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TWI635624B - Semiconductor light emitting element and method of manufacturing same - Google Patents

Semiconductor light emitting element and method of manufacturing same Download PDF

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TWI635624B
TWI635624B TW103125809A TW103125809A TWI635624B TW I635624 B TWI635624 B TW I635624B TW 103125809 A TW103125809 A TW 103125809A TW 103125809 A TW103125809 A TW 103125809A TW I635624 B TWI635624 B TW I635624B
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light
layer
emitting device
semiconductor light
semiconductor
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TW201519468A (en
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井上振一郎
溜直樹
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國立研究開發法人情報通信研究機構
斯坦雷電氣股份有限公司
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/85Packages
    • H10H20/855Optical field-shaping means, e.g. lenses
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/01Manufacture or treatment
    • H10H20/011Manufacture or treatment of bodies, e.g. forming semiconductor layers
    • H10H20/013Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/819Bodies characterised by their shape, e.g. curved or truncated substrates
    • H10H20/82Roughened surfaces, e.g. at the interface between epitaxial layers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/01Manufacture or treatment
    • H10H20/036Manufacture or treatment of packages
    • H10H20/0363Manufacture or treatment of packages of optical field-shaping means
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/822Materials of the light-emitting regions
    • H10H20/824Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
    • H10H20/825Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/872Periodic patterns for optical field-shaping, e.g. photonic bandgap structures

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Abstract

本發明提供即使發光波長短亦可獲得光取出效率高、均一的光輸出的半導體發光元件、以及可以高再現性、高產量製造此半導體發光元件的半導體發光元件的製造方法。半導體發光元件,是具有含發光層的半導體層之半導體發光元件,半導體發光元件的表面包含光取出面。在光取出面及半導體發光元件內折射率互異的二層的界面的至少任一個,形成有:週期凹凸構造,具有比從發光層發射的光的波長的0.5倍還大的週期;以及微細凹凸構造,位於週期凹凸構造的表面上,具有光的波長的0.5倍以下的平均直徑。 The present invention provides a semiconductor light-emitting device which can obtain a light extraction efficiency with high light extraction efficiency even when the light-emitting wavelength is short, and a method of manufacturing a semiconductor light-emitting device which can manufacture the semiconductor light-emitting device with high reproducibility and high yield. The semiconductor light emitting element is a semiconductor light emitting element having a semiconductor layer including a light emitting layer, and the surface of the semiconductor light emitting element includes a light extraction surface. At least one of the interfaces of the two layers having different refractive indices in the light extraction surface and the semiconductor light emitting element is formed with a periodic uneven structure having a period larger than 0.5 times the wavelength of light emitted from the light emitting layer; and fine The uneven structure is located on the surface of the periodic concavo-convex structure and has an average diameter of 0.5 times or less of the wavelength of light.

Description

半導體發光元件及其製造方法 Semiconductor light emitting element and method of manufacturing same

本發明是關於發光二極體(LED)等的半導體發光元件,特別是關於為了針對以元件內發出的光通向外部之光取出作改善的半導體發光元件及其製造方法。 The present invention relates to a semiconductor light-emitting element such as a light-emitting diode (LED), and more particularly to a semiconductor light-emitting element for improving light extraction to the outside through light emitted from the element, and a method of manufacturing the same.

半導體發光元件是由發光層、n型半導體層、p型半導體層、電極層、支持基板等數層而形成。因此,以半導體元件內部的發光層發出的光,是通過這些數層之後被取出至外部。然而,關於光,在通過折射率不同的介質的交界也就是層界面、表面等之時,必定會發生既定比例的反射。另外,光通過對上述光的波長(發光波長)具有吸收係數的介質層或反射之時,會發生既定比例的光吸收。因此,要有效率地將以發光層發出的光取出至半導體發光元件的外部,一般而言是困難的。 The semiconductor light emitting element is formed of a plurality of layers such as a light emitting layer, an n-type semiconductor layer, a p-type semiconductor layer, an electrode layer, and a supporting substrate. Therefore, the light emitted from the light-emitting layer inside the semiconductor element is taken out to the outside through these several layers. However, with regard to light, when passing through the boundary of a medium having a different refractive index, that is, a layer interface, a surface, or the like, a predetermined ratio of reflection must occur. Further, when light passes through a dielectric layer having an absorption coefficient for the wavelength (light emission wavelength) of the light or is reflected, light absorption of a predetermined ratio occurs. Therefore, it is generally difficult to efficiently extract light emitted from the light-emitting layer to the outside of the semiconductor light-emitting element.

特別是光從折射率大的介質進到折射率小的介質時,會引起光的全反射,臨界角以上的光無法取出至外部。在半導體發光元件的表面、也就是空氣(或密封材料)與半導體元件的界面,由於兩介質間的折射率大,引起全反射的臨界角小,結果在界面被全反射的光的比例增大。 In particular, when light enters a medium having a large refractive index from a medium having a large refractive index, total light is totally reflected, and light having a critical angle or higher cannot be taken out to the outside. At the interface of the semiconductor light-emitting element, that is, the interface between the air (or sealing material) and the semiconductor element, since the refractive index between the two mediums is large, the critical angle of total reflection is small, and as a result, the proportion of light totally reflected at the interface is increased. .

例如藍寶石基板的折射率n為1.8,對空氣的臨界角為33.7度。亦即,使用藍寶石作為構成半導體發光元件的基板 時、通過藍寶石基板向空氣側取出光線時,入射角大於33.7度的光會被全反射而無法被取出到外界。甚至折射率大的氮化鋁(AlN)基板(折射率n=2.29)的情況,臨界角成為25.9度,僅有更少的光能夠取出至外部。 For example, the sapphire substrate has a refractive index n of 1.8 and a critical angle to air of 33.7 degrees. That is, sapphire is used as a substrate constituting the semiconductor light-emitting element When light is taken out to the air side through the sapphire substrate, light having an incident angle of more than 33.7 degrees is totally reflected and cannot be taken out to the outside. Even in the case of an aluminum nitride (AlN) substrate having a large refractive index (refractive index n = 2.29), the critical angle is 25.9 degrees, and only less light can be taken out to the outside.

使用利用三次元時域有限差分法(Finite-Difference Time-Domain method;FDTD法)的光放射傳播特性的理論計算,計算例如在AlN基板上層積AlGaN層的半導體發光元件中的光的取出效率。其結果,若亦考慮從AlGaN層內的發光部放射的波長265nm的光之內、位於從發光部所見與AlN基板為相反側的p型GaN層的吸收等,從AlN基板的表面(光取出面)側可以取出的光的取出效率極低,為約4%。 The light extraction efficiency of the semiconductor light-emitting element in which the AlGaN layer is laminated on the AlN substrate is calculated using theoretical calculation of the light emission characteristics by the Finite-Difference Time-Domain Method (FDTD method). As a result, the surface of the AlN substrate (light extraction) is taken into consideration from the light having a wavelength of 265 nm emitted from the light-emitting portion in the AlGaN layer and the absorption of the p-type GaN layer on the opposite side to the AlN substrate as seen from the light-emitting portion. The extraction efficiency of light that can be taken out on the side of the surface is extremely low, about 4%.

對於這樣的問題,以提升光取出效率為目的,有人提出在基板表面(光取出面)設置奈米尺度的凹凸構造的半導體發光元件。例如在專利文獻1中,揭露將具有藉由發光層發出的光的平均光學波長的2倍以下的平均週期的凹凸構造設於光取出面。藉由形成這樣的凹凸構成,提出減低在光取出面被全反射的光的部分的比例(亦即抑制在元件表面的光的反射)的方法。然而,在半導體發光元件的表面形成奈米尺度的凹凸構造,並不容易。另外,根據凹凸構造的形狀、發光波長等,光取出效率亦會大幅變動,無法獲得充分的效果。 For such a problem, in order to enhance the light extraction efficiency, a semiconductor light-emitting element having a nano-scale uneven structure on the substrate surface (light extraction surface) has been proposed. For example, in Patent Document 1, it is disclosed that an uneven structure having an average period of twice or less the average optical wavelength of light emitted from the light-emitting layer is provided on the light extraction surface. By forming such a concavo-convex structure, a method of reducing the ratio of the portion of the light that is totally reflected on the light extraction surface (that is, suppressing the reflection of light on the surface of the element) is proposed. However, it is not easy to form a nano-scale uneven structure on the surface of the semiconductor light-emitting element. In addition, depending on the shape of the uneven structure, the wavelength of light emission, and the like, the light extraction efficiency also largely changes, and a sufficient effect cannot be obtained.

由於發光波長變得愈短,所要求的凹凸構造的週期(例如凸構造的情況,凸構造的頂點部與鄰接的凸構造的頂點部為止的距離)就變得愈短,此凹凸構造的製作就變得困難。特別是發出紫外.深紫外波長區域的光的半導體發光元件 中,此凹凸構造的尺寸會成為以光微影法製作困難的領域。其結果,因為發生製作成本的增加、良率、產量變低等的問題,而無實用性。 The shorter the light-emitting wavelength is, the shorter the period of the desired uneven structure (for example, the convex structure, the distance between the apex portion of the convex structure and the apex portion of the adjacent convex structure) is shorter, and the uneven structure is produced. It becomes difficult. Especially emitting ultraviolet light. Semiconductor light-emitting elements of light in the deep ultraviolet wavelength region In this case, the size of the uneven structure becomes a field in which it is difficult to manufacture by photolithography. As a result, problems such as an increase in production cost, a decrease in yield, and a low yield occur, and there is no practicality.

在專利文獻1(特開2005-354020號公報)中,揭露為了形成奈米尺度的週期凹凸構造,在光取出面上形成將已蒸鍍的金屬加熱而使其凝集的奈米尺度的微細金屬罩幕、蝕刻此光取出面的表面的方法。然而利用這樣的凝集效果的週期罩幕,凹凸構造的配置為無序,其形狀的不均一性大。因此,從半導體發光元件輸出至外部的光的功率的變異度大,難以提供發射穩定、均質的光的半導體發光元件。 In order to form a periodic uneven structure of a nanometer scale, a nanometer-scale fine metal in which a vapor-deposited metal is heated and aggregated is formed on a light extraction surface in the patent document 1 (JP-A-2005-354020). A method of masking the surface of the light extraction surface. However, with the periodic mask having such an agglomeration effect, the arrangement of the concavo-convex structure is disordered, and the shape unevenness is large. Therefore, the degree of variation in the power of light output from the semiconductor light emitting element to the outside is large, and it is difficult to provide a semiconductor light emitting element that emits stable and uniform light.

在非專利文獻1(ISDRS 2011,December 7-9,2011,College Park,MD,USA,WP2-04)中,揭露為了形成奈米尺度的凹凸構造,藉由溼蝕刻將基板表面粗面化的方法。然而,藉由使用溼蝕刻的手法而形成的凹凸構造亦由於成為形狀不均一的無序構造,光取出效率大幅變動,且光取出效率提升的效果亦不充分。 In Non-Patent Document 1 (ISDRS 2011, December 7-9, 2011, College Park, MD, USA, WP2-04), it is disclosed that the surface of the substrate is roughened by wet etching in order to form a concave-convex structure of a nanometer scale. method. However, the uneven structure formed by the wet etching method is also a disordered structure having a non-uniform shape, and the light extraction efficiency greatly fluctuates, and the effect of improving the light extraction efficiency is also insufficient.

在非專利文獻2(Appl.Phys.Express 3(2010)061004)中,在發射深紫外的光的半導體發光元件中,藉由微影、乾蝕刻設置表面週期凹凸構造,但此凹凸構造的週期為500nm,是發光波長2倍程度大,無法得到光取出效率提升的充分效果。另外,光輸出的變異度亦極大。 In Non-Patent Document 2 (Appl. Phys. Express 3 (2010) 061004), in a semiconductor light-emitting element that emits deep ultraviolet light, a surface periodic uneven structure is provided by lithography or dry etching, but the period of the uneven structure is When the wavelength is 500 nm, the wavelength of the light is twice as large, and the sufficient effect of improving the light extraction efficiency cannot be obtained. In addition, the variability of the light output is also extremely large.

【先行技術文獻】 [First technical literature]

【專利文獻】 [Patent Literature]

【專利文獻1】特開2005-354020號公報 [Patent Document 1] JP-A-2005-354020

【非專利文獻】 [Non-patent literature]

【非專利文獻1】ISDRS 2011, December 7-9, 2011, College Park, MD, USA, WP2-04 [Non-Patent Document 1] ISDRS 2011, December 7-9, 2011, College Park, MD, USA, WP2-04

【非專利文獻2】Appl. Phys. Express 3(2010)061004 [Non-Patent Document 2] Appl. Phys. Express 3 (2010) 061004

如上所述,在基板表面(光取出面)設置奈米尺度的凹凸構造的半導體發光元件,是以提升光取出效率為目的而被提出,但在這樣的習知的發光元件中,凹凸構造的週期、構成凹凸構造的凸部的高度、形狀等的最佳值並不明確且會根據發光波長、基板的折射率等而變動,無法發揮充分的效果是為現狀。還有,隨著發光波長變為短波長,由於有必要在基板表面(光取出面)形成更小尺度的凹凸構造,此凹凸構造的製作便更加困難。因此,即使發光波長為短波長,仍以良好再現性、均一地形成使光取出效率充分提升的凹凸構造,而進一步使從半導體發光元件輸出至外部的光的功率均一化、安定化為很大的課題。 As described above, a semiconductor light-emitting element having a nano-scale uneven structure on the surface of the substrate (light extraction surface) is proposed for the purpose of improving light extraction efficiency. However, in such a conventional light-emitting element, the uneven structure is provided. The optimum value of the period and the height and shape of the convex portion constituting the uneven structure is not clear and varies depending on the light-emitting wavelength, the refractive index of the substrate, and the like, and it is a state in which a sufficient effect cannot be exhibited. Further, as the emission wavelength becomes a short wavelength, it is necessary to form a concavo-convex structure having a smaller dimension on the surface (light extraction surface) of the substrate, which makes it more difficult to fabricate the concavo-convex structure. Therefore, even if the light-emitting wavelength is a short wavelength, the uneven structure in which the light extraction efficiency is sufficiently improved is formed with good reproducibility, and the power output from the semiconductor light-emitting element to the outside is further uniformized and stabilized. Question.

因此,本發明的目的是為了解決如上述的習知課題,而提供即使發光波長短亦可獲得光取出效率高、均一的光輸出的半導體發光元件、以及可以高再現性、高產量製造此半導體發光元件的半導體發光元件的製造方法。 Therefore, an object of the present invention is to provide a semiconductor light-emitting element which can obtain a light extraction efficiency with high light extraction efficiency and a uniform light output, and can manufacture the semiconductor with high reproducibility and high yield, even if the light-emitting wavelength is short. A method of manufacturing a semiconductor light-emitting device of a light-emitting element.

根據本發明的半導體發光元件,是具有含發光層的半導體層之半導體發光元件,半導體發光元件的表面包含光取出面。在光取出面及半導體發光元件內折射率互異的二層的界面的至少任一個,形成有:週期凹凸構造,具有比從發光層發射的光的波長的0.5倍還大的週期;以及微細凹凸構造,位於週期凹凸構造的表面上,具有光的波長的0.5倍以下的平均直徑。 A semiconductor light emitting device according to the present invention is a semiconductor light emitting element having a semiconductor layer containing a light emitting layer, and a surface of the semiconductor light emitting element includes a light extraction surface. At least one of the interfaces of the two layers having different refractive indices in the light extraction surface and the semiconductor light emitting element is formed with a periodic uneven structure having a period larger than 0.5 times the wavelength of light emitted from the light emitting layer; and fine The uneven structure is located on the surface of the periodic concavo-convex structure and has an average diameter of 0.5 times or less of the wavelength of light.

藉由本發明,可以得到獲得高的光取出效率的半導體發光元件。 According to the present invention, a semiconductor light-emitting element which achieves high light extraction efficiency can be obtained.

11‧‧‧正電極 11‧‧‧ positive electrode

12‧‧‧p型半導體層 12‧‧‧p-type semiconductor layer

13‧‧‧活性層 13‧‧‧Active layer

14‧‧‧負電極 14‧‧‧Negative electrode

15‧‧‧n型半導體層 15‧‧‧n type semiconductor layer

16‧‧‧基板 16‧‧‧Substrate

16A‧‧‧背面 16A‧‧‧Back

21‧‧‧週期凹凸構造 21‧‧‧Cycle relief structure

22‧‧‧微細凹凸構造 22‧‧‧Micro-concave structure

D1、D2‧‧‧直徑 D1, D2‧‧‧ diameter

H1‧‧‧高度 H1‧‧‧ Height

L1‧‧‧週期 L1‧‧ cycle

S10、S100‧‧‧基板準備步驟 S10, S100‧‧‧ substrate preparation steps

S20、S200‧‧‧半導體層形成步驟 S20, S200‧‧‧ semiconductor layer formation steps

S30、S300‧‧‧電極形成步驟 S30, S300‧‧‧ electrode formation steps

S40、S400‧‧‧凹凸構造形成步驟 S40, S400‧‧‧ concave and convex structure forming steps

S41‧‧‧罩幕形成步驟 S41‧‧‧ Cover forming steps

S42、S420‧‧‧蝕刻步驟 S42, S420‧‧‧ etching steps

S43‧‧‧罩幕移除步驟 S43‧‧‧ Mask removal steps

S410‧‧‧蝕刻罩幕製作步驟 S410‧‧‧ Etching mask production steps

S430‧‧‧蝕刻罩幕移除步驟 S430‧‧‧ Etching mask removal steps

第1圖是本發明相關的半導體發光元件的實施的形態1的剖面模式圖。 Fig. 1 is a schematic cross-sectional view showing a first embodiment of a semiconductor light emitting device according to the present invention.

第2圖是示於第1圖的半導體發光元件的光取出面的平面模式圖。 Fig. 2 is a plan schematic view showing a light extraction surface of the semiconductor light emitting element shown in Fig. 1.

第3圖是在第2圖的線段III-III的部分剖面模式圖。 Fig. 3 is a partial cross-sectional schematic view of line segment III-III in Fig. 2;

第4圖是用以說明示於第1圖的半導體發光元件的變形例之平面模式圖。 Fig. 4 is a plan schematic view for explaining a modification of the semiconductor light emitting element shown in Fig. 1.

第5圖是用以說明示於第1圖的半導體發光元件的製造方法之流程圖。 Fig. 5 is a flow chart for explaining a method of manufacturing the semiconductor light emitting element shown in Fig. 1.

第6圖是用以說明本發明相關的半導體發光元件的實施的形態2的平面模式圖。 Fig. 6 is a plan schematic view showing a second embodiment of the semiconductor light emitting device according to the present invention.

第7圖是在第6圖的線段VII-VII的部分剖面模式圖。 Fig. 7 is a partial cross-sectional schematic view of line VII-VII of Fig. 6.

第8圖是用以說明示於第6圖的半導體發光元件的變形例之平面模式圖。 Fig. 8 is a plan schematic view for explaining a modification of the semiconductor light emitting element shown in Fig. 6.

第9圖是用以說明示於第6圖的半導體發光元件的製造方法之流程圖。 Fig. 9 is a flow chart for explaining a method of manufacturing the semiconductor light emitting element shown in Fig. 6.

第10圖是用作實施例1的試樣的半導體發光元件之平面模式圖。 Fig. 10 is a plan view schematically showing a semiconductor light emitting element used as a sample of Example 1.

第11圖是在第10圖的線段XI-XI的剖面模式圖。 Fig. 11 is a schematic cross-sectional view of the line segment XI-XI of Fig. 10.

第12圖是示於第10圖的半導體發光元件的光取出面的掃描式電子顯微鏡照片。 Fig. 12 is a scanning electron micrograph of the light extraction surface of the semiconductor light emitting element shown in Fig. 10.

第13圖是示於第10圖的半導體發光元件的光取出面的掃描式電子顯微鏡照片。 Fig. 13 is a scanning electron micrograph of the light extraction surface of the semiconductor light emitting element shown in Fig. 10.

第14圖是顯示實施例1的實驗結果的圖表。 Fig. 14 is a graph showing the results of the experiment of Example 1.

第15圖是用作實施例2的試樣的半導體發光元件的光取出面之掃描式電子顯微鏡照片。 Fig. 15 is a scanning electron micrograph of the light extraction surface of the semiconductor light emitting element used as the sample of Example 2.

第16圖是用作實施例2的試樣的半導體發光元件的光取出面之掃描式電子顯微鏡照片。 Fig. 16 is a scanning electron micrograph of the light extraction surface of the semiconductor light emitting element used as the sample of Example 2.

第17圖是用作實施例2的試樣的半導體發光元件的光取出面之掃描式電子顯微鏡照片。 Fig. 17 is a scanning electron micrograph of the light extraction surface of the semiconductor light emitting element used as the sample of Example 2.

第18圖是顯示實施例1的實驗結果的圖表。 Fig. 18 is a graph showing the results of the experiment of Example 1.

第19圖是顯示實施例3的模擬計算結果的圖表。 Fig. 19 is a graph showing the results of the simulation calculation of the third embodiment.

第20圖是顯示實施例3的模擬計算結果的圖表。 Fig. 20 is a graph showing the results of the simulation calculation of Example 3.

第21圖是顯示實施例4的模擬計算結果的圖表。 Fig. 21 is a graph showing the results of the simulation calculation of Example 4.

第22圖是顯示實施例4的模擬計算結果的圖表。 Fig. 22 is a graph showing the results of the simulation calculation of Example 4.

第23圖是顯示實施例5的實驗結果的圖表。 Fig. 23 is a graph showing the results of the experiment of Example 5.

第24圖是顯示實施例6的實驗結果的圖表。 Fig. 24 is a graph showing the results of the experiment of Example 6.

第25圖是顯示實施例7的實驗結果的圖表。 Fig. 25 is a graph showing the experimental results of Example 7.

第26圖是顯示實施例8及實施例9的實驗結果的圖表。 Fig. 26 is a graph showing the results of experiments of Example 8 and Example 9.

第27圖是顯示實施例中的實驗值與模擬計算結果的圖表。 Figure 27 is a graph showing experimental values and simulation calculation results in the examples.

【用以實施發明的形態】 [Formation for implementing the invention]

首先,針對實施的形態的概要作說明。 First, an outline of the form of implementation will be described.

(1)根據本實施形態之半導體發光元件,是具有含發光層(活性層13)的半導體層之半導體發光元件,半導體發光元件的表面包含光取出面。在光取出面及半導體發光元件內折射率互異的二層的界面的至少任一個,形成有:週期凹凸構造21,具有比從發光層發射的光的波長的0.5倍還大的週期;以及微細凹凸構造22,位於週期凹凸構造21的表面上,具有光的波長的0.5倍以下的平均直徑。 (1) The semiconductor light-emitting device according to the present embodiment is a semiconductor light-emitting device having a semiconductor layer including a light-emitting layer (active layer 13), and the surface of the semiconductor light-emitting device includes a light extraction surface. At least one of the interfaces of the two layers having different refractive indices in the light extraction surface and the semiconductor light emitting element is formed with a periodic uneven structure 21 having a period larger than 0.5 times the wavelength of light emitted from the light emitting layer; The fine concavo-convex structure 22 is located on the surface of the periodic concavo-convex structure 21 and has an average diameter of 0.5 times or less of the wavelength of light.

若是如此,由於在光取出面中形成因應從發光層發射的光的波長(發光波長)的週期的週期凹凸構造21及具有因應此波長的平均直徑的微細凹凸構造22,與在光取出面無這些凹凸構造的情況比較,可確實地提高光取出效率。亦即,即使是形成週期大於波長的週期凹凸構造的情況,藉由與微細凹凸構造組合,可以充分地提升光取出效率。進一步,發光波長為短波長(例如450nm以下、或是350nm以下)時,在根據本實施形態之半導體發光元件中,抑制週期凹凸構造的製造相關的成本的增加之效果變得顯著。另外,由於可以以比週期凹凸構造的發光波長還大的週期形成,均一的凹凸構造的形成則變得容 易。 In this case, the periodic concavo-convex structure 21 having a period corresponding to the wavelength (emission wavelength) of the light emitted from the light-emitting layer and the fine concavo-convex structure 22 having an average diameter corresponding to the wavelength are formed in the light extraction surface, and there is no In comparison with the case of these uneven structures, the light extraction efficiency can be surely improved. In other words, even in the case of forming a periodic uneven structure having a period larger than the wavelength, the light extraction efficiency can be sufficiently improved by combining with the fine uneven structure. Further, when the light-emitting wavelength is a short wavelength (for example, 450 nm or less or 350 nm or less), the semiconductor light-emitting device according to the present embodiment has an effect of suppressing an increase in cost associated with the production of the periodic uneven structure. In addition, since it can be formed at a period larger than the emission wavelength of the periodic uneven structure, the formation of a uniform uneven structure becomes uniform. easy.

(2)在上述半導體發光元件中,週期凹凸構造21的排列圖形可為三角格子狀。此時,週期凹凸構造21的凸形狀部的每單位面積的數量可容易變多。 (2) In the above semiconductor light emitting element, the arrangement pattern of the periodic uneven structure 21 may be a triangular lattice shape. At this time, the number of the convex portions of the periodic concavo-convex structure 21 per unit area can be easily increased.

(3)在上述半導體發光元件中,週期凹凸構造21可包含由折射率高於空氣的高折射率材料部構成的凸部(凸形狀部)。在對於從發光層(活性層13)向上述光取出面(基板16的背面16A)的方向垂直的面的凸部的截面積,可隨著遠離發光層(活性層13)而變小。若是如此,光取出面的外部介質為空氣時,可確實地提高從光取出面的光取出效率。 (3) In the above semiconductor light emitting device, the periodic concavo-convex structure 21 may include a convex portion (convex portion) composed of a high refractive index material portion having a refractive index higher than that of air. The cross-sectional area of the convex portion on the surface perpendicular to the direction from the light-emitting layer (active layer 13) to the light extraction surface (back surface 16A of the substrate 16) can be made smaller as it goes away from the light-emitting layer (active layer 13). If the external medium of the light extraction surface is air, the light extraction efficiency from the light extraction surface can be surely improved.

(4)在上述半導體發光元件中,凸部的形狀可為錐體形狀或半橢圓球形狀。此時,使用蝕刻等比較一般性的製程可容易地形成凸部。 (4) In the above semiconductor light emitting element, the shape of the convex portion may be a pyramid shape or a semi-elliptical spherical shape. At this time, the convex portion can be easily formed using a relatively general process such as etching.

(5)在上述半導體發光元件中,發光層可含III族氮化物半導體。半導體層可含:導電型為n型的n型III族氮化物半導體層(n型半導體層15);以及導電型為p型的p型III族氮化物半導體層(p型半導體層12),位於從發光層所見與n型III族氮化物半導體層的相反側。若使用這樣的III族氮化物半導體,可以獲得發射發光波長為450nm以下之所謂的短波長的光的半導體發光元件。 (5) In the above semiconductor light emitting element, the light emitting layer may contain a group III nitride semiconductor. The semiconductor layer may include: an n-type group III nitride semiconductor layer (n-type semiconductor layer 15) having a conductivity type of n-type; and a p-type group III nitride semiconductor layer (p-type semiconductor layer 12) having a conductivity type of p-type, Located on the opposite side of the n-type group III nitride semiconductor layer as seen from the light-emitting layer. When such a group III nitride semiconductor is used, a semiconductor light-emitting element that emits light of a so-called short wavelength having an emission wavelength of 450 nm or less can be obtained.

(6)上述半導體發光元件,可具有一透明性基板,配置於從發光層到光取出面側,對從發光層發射的光具有透明性。此時,可以將透明基板的背面(與形成有半導體層的主表面為相反側的背面)作為光取出面來使用。 (6) The semiconductor light-emitting device may have a transparent substrate disposed on the side from the light-emitting layer to the light extraction surface and having transparency to light emitted from the light-emitting layer. At this time, the back surface of the transparent substrate (the back surface opposite to the main surface on which the semiconductor layer is formed) can be used as the light extraction surface.

(7)在上述半導體發光元件中,透明性基板可為氮化鋁基板。此時,可以大幅減低含由III族氮化物半導體構成的發光層的半導體層的缺陷密度。 (7) In the above semiconductor light emitting device, the transparent substrate may be an aluminum nitride substrate. At this time, the defect density of the semiconductor layer containing the light-emitting layer composed of the group III nitride semiconductor can be greatly reduced.

(8)在上述半導體發光元件中,從發光層發射的光的波長可為450nm以下。這樣的發光波長為短波長時,可以顯著地獲得如上述的效果。 (8) In the above semiconductor light emitting element, the wavelength of light emitted from the light emitting layer may be 450 nm or less. When such an emission wavelength is a short wavelength, the effects as described above can be remarkably obtained.

(9)在上述半導體發光元件中,週期凹凸構造21的高度H1相對於週期凹凸構造21的週期L1可為1/3倍以上、5倍以下;微細凹凸構造22的平均高度相對於微細凹凸構造22的平均直徑可為0.1倍以上、10倍以下。此時,可以確實地提升光取出效率。 (9) In the semiconductor light-emitting device, the height H1 of the periodic concavo-convex structure 21 may be 1/3 times or more and 5 times or less with respect to the period L1 of the periodic concavo-convex structure 21; and the average height of the fine concavo-convex structure 22 is relative to the fine concavo-convex structure The average diameter of 22 may be 0.1 times or more and 10 times or less. At this time, the light extraction efficiency can be surely improved.

(10)根據本實施形態之半導體發光元件,包含:氮化鋁構成的基板16;以及形成於基板16的主表面上的半導體層。半導體層包含:含III族氮化物半導體的發光層(活性層13)、配置為夾置發光層之導電型為n型的n型III族氮化物半導體層(n型半導體層15)及導電型為p型的p型III族氮化物半導體層(p型半導體層12)。從發光層發射的光的波長為350nm以下。在基板16位於與主表面為相反側的背面,形成有一週期凹凸構造21,週期凹凸構造21具有一週期,上述週期為從發光層發射的光的波長除以構成基板的氮化鋁的折射率與位於基板的外部的外部介質的折射率的差之值(評量值)的1/3倍以上、5倍以下。 (10) The semiconductor light emitting device according to the present embodiment includes: a substrate 16 made of aluminum nitride; and a semiconductor layer formed on a main surface of the substrate 16. The semiconductor layer includes a light-emitting layer (active layer 13) containing a group III nitride semiconductor, an n-type group III nitride semiconductor layer (n-type semiconductor layer 15) having a conductivity type in which a light-emitting layer is interposed, and a conductive type. It is a p-type p-type group III nitride semiconductor layer (p-type semiconductor layer 12). The wavelength of light emitted from the light-emitting layer is 350 nm or less. On the back surface of the substrate 16 on the opposite side to the main surface, a periodic concavo-convex structure 21 having a period in which the wavelength of light emitted from the light-emitting layer is divided by the refractive index of the aluminum nitride constituting the substrate is formed is formed. The value (measured value) of the difference in refractive index of the external medium located outside the substrate is 1/3 times or more and 5 times or less.

此時,由於按照從發光層發射的光的波長(發光波長)、由AlN構成的基板16的折射率、與外部介質的折射率決定 週期凹凸構造21的週期,可以確實地提升從基板16的背面(光取出面)的光取出效率。 At this time, it is determined by the wavelength (light emission wavelength) of light emitted from the light-emitting layer, the refractive index of the substrate 16 composed of AlN, and the refractive index of the external medium. The period of the periodic concavo-convex structure 21 can surely improve the light extraction efficiency from the back surface (light extraction surface) of the substrate 16.

另外,上述週期較好為評量值的0.5倍以上、4倍以下,更好為1倍以上、3倍以下。 Further, the period is preferably 0.5 times or more and 4 times or less, more preferably 1 time or more and 3 times or less the evaluation value.

(11)在上述半導體發光元件中,週期凹凸構造21的排列圖形可為三角格子狀。此時,週期凹凸構造21的凸形狀部的每單位面積的數量可容易變多。 (11) In the above semiconductor light emitting device, the arrangement pattern of the periodic uneven structure 21 may be a triangular lattice shape. At this time, the number of the convex portions of the periodic concavo-convex structure 21 per unit area can be easily increased.

(12)在上述半導體發光元件中,週期凹凸構造包含凸部,凸部的形狀可為錐體形狀或半橢圓球形狀。此時,使用蝕刻等比較一般性的製程可容易地形成凸部。 (12) In the above semiconductor light emitting device, the periodic concavo-convex structure includes a convex portion, and the shape of the convex portion may be a pyramid shape or a semi-elliptical spherical shape. At this time, the convex portion can be easily formed using a relatively general process such as etching.

(13)在上述半導體發光元件中,週期凹凸構造的高度相對於週期凹凸構造的週期可為1/3倍以上、5倍以下。此時,可以確實地提升光取出效率。 (13) In the semiconductor light-emitting device, the height of the periodic concavo-convex structure may be 1/3 times or more and 5 times or less with respect to the period of the periodic concavo-convex structure. At this time, the light extraction efficiency can be surely improved.

另外,上述高度較好為評量值的0.5倍以上、2倍以下,更好為0.6倍以上、1.8倍以下。 Further, the height is preferably 0.5 times or more and 2 times or less, more preferably 0.6 times or more and 1.8 times or less.

(14)根據本實施形態之半導體發光元件的製造方法,包含下列步驟:準備即將成為包含具有發光層的半導體層的半導體發光元件的元件構件;在上述元件構件,在即將成為上述半導體發光元件的光取出面的區域上,形成具有圖形的罩幕層;以及以上述罩幕層為罩幕,藉由蝕刻部分性地移除上述即將成為光取出面的區域,藉此形成週期凹凸構造。罩幕層為金屬罩幕層。在形成週期凹凸構造的步驟中,是藉由進行使用氟系氣體作為蝕刻氣體的乾蝕刻,形成週期凹凸構造,並在移除前述罩幕層的殘渣的步驟中,在週期凹凸構造的表面形成微 細凹凸構造。週期凹凸構造,具有超過從發光層發射的光的波長的0.5倍的週期。微細凹凸構造具有光的波長的0.5倍以下的平均直徑。另外,以週期凹凸構造與微細凹凸構造為由相同材質構成為特徵。若是如此,可以容易獲得根據本實施形態之半導體發光元件。 (14) A method of manufacturing a semiconductor light-emitting device according to the present embodiment, comprising the steps of: preparing an element member to be a semiconductor light-emitting element including a semiconductor layer having a light-emitting layer; and the element member immediately becoming the semiconductor light-emitting element A mask layer having a pattern is formed on the light extraction surface; and the mask layer is used as a mask to partially remove the region to be the light extraction surface by etching, thereby forming a periodic uneven structure. The mask layer is a metal mask layer. In the step of forming the periodic concavo-convex structure, a periodic uneven structure is formed by dry etching using a fluorine-based gas as an etching gas, and in the step of removing the residue of the mask layer, a surface of the periodic concavo-convex structure is formed. micro- Fine concave and convex construction. The periodic concavo-convex structure has a period exceeding 0.5 times the wavelength of light emitted from the luminescent layer. The fine concavo-convex structure has an average diameter of 0.5 times or less of the wavelength of light. Further, the periodic concavo-convex structure and the fine concavo-convex structure are characterized by the same material. If so, the semiconductor light emitting element according to the embodiment can be easily obtained.

(15)根據本實施形態之半導體發光元件的製造方法,包含下列步驟:準備即將成為半導體發光元件的元件構件,上述半導體發光元件包含氮化鋁構成的基板、與形成於此基板的主表面上且具有發光層的半導體層;在元件構件,在即將成為半導體發光元件的光取出面的區域上,形成具有圖形的罩幕層;以及以罩幕層為罩幕,藉由蝕刻部分性地移除上述即將成為光取出面的區域,藉此形成週期凹凸構造。週期凹凸構造具有一週期,上述週期為從發光層發射的光的波長除以構成基板的氮化鋁的折射率與位於基板的外部的外部介質的折射率的差之值的1/3倍以上、5倍以下。若是如此,可以容易獲得根據本實施形態之半導體發光元件。 (15) A method of manufacturing a semiconductor light-emitting device according to the present embodiment, comprising the steps of: preparing an element member to be a semiconductor light-emitting element, wherein the semiconductor light-emitting element comprises a substrate made of aluminum nitride, and a main surface formed on the substrate And a semiconductor layer having a light-emitting layer; in the element member, a mask layer having a pattern is formed on a region to be a light extraction surface of the semiconductor light-emitting element; and a mask is used as a mask to partially shift by etching In addition to the above-described region which is to be the light extraction surface, a periodic uneven structure is formed thereby. The periodic concavo-convex structure has a period in which the wavelength of light emitted from the light-emitting layer is divided by more than 1/3 times the value of the difference between the refractive index of the aluminum nitride constituting the substrate and the refractive index of the external medium located outside the substrate. , 5 times or less. If so, the semiconductor light emitting element according to the embodiment can be easily obtained.

(16)在上述半導體發光元件中,週期凹凸構造21的週期,可為光的波長的1倍以上。此時,可容易製造週期凹凸構造21。 (16) In the above semiconductor light-emitting device, the period of the periodic concavo-convex structure 21 may be one time or more of the wavelength of light. At this time, the periodic uneven structure 21 can be easily manufactured.

(17)在上述半導體發光元件中,週期凹凸構造21的週期,可為光的波長的2倍以上。另外,微細凹凸構造22的平均直徑,可為光的波長的0.4倍以下。此時,可避免半導體發光元件的製造成本的增加,還可確實地提高光取出效率。 (17) In the above semiconductor light-emitting device, the period of the periodic concavo-convex structure 21 may be twice or more the wavelength of light. Further, the average diameter of the fine concavo-convex structure 22 may be 0.4 times or less the wavelength of light. At this time, an increase in the manufacturing cost of the semiconductor light emitting element can be avoided, and the light extraction efficiency can be surely improved.

(18)在上述半導體發光元件中,透明性基板可為藍 寶石基板。即使為這樣的構成,仍可獲得已提高光取出效率的半導體發光元件。 (18) In the above semiconductor light emitting element, the transparent substrate may be blue Gem substrate. Even with such a configuration, a semiconductor light emitting element having improved light extraction efficiency can be obtained.

(19)在上述半導體發光元件中,從發光層發射的光的波長(發光波長)可為350nm以下。此時,在發射如上述的短波長的光的半導體發光元件,根據本實施形態之效果是顯著的。 (19) In the above semiconductor light emitting device, the wavelength (light emission wavelength) of light emitted from the light emitting layer may be 350 nm or less. At this time, the effect of the present embodiment is remarkable in the semiconductor light-emitting device that emits light of a short wavelength as described above.

接下來,針對發明的實施的形態的具體例,參照適當圖式作說明。不過,以下說明的發光元件,是為了將本發明的技術思想具體化者,而非將本發明限定在以下的元件。特別是以下揭露的構成構件的尺寸、材質、形狀、其相對性配置等只要無特定的記載,其宗旨並非將本發明的範圍限定在僅是上述情況,而僅為單純的說明例。另外,各圖式所示的零件的大小、位置關係等,會有為了明確地作說明而誇大的情況。另外,構成本發明的各元件,可以是以同一零件構成複數個元件而作為以一個零件兼用複數個元件的樣態,亦可以是相反地以複數個零件分擔實現一個零件的功能。還有,針對以下揭露的各實施例,亦同樣地只要無特別排除的記載,可以適當組合各構成等而應用。 Next, a specific example of the form of the embodiment of the invention will be described with reference to the appropriate drawings. However, the light-emitting elements described below are intended to embody the technical idea of the present invention, and are not intended to limit the present invention to the following elements. In particular, the dimensions, materials, shapes, relative positions, and the like of the constituent members disclosed below are not intended to limit the scope of the present invention to the above-described case, and are merely illustrative examples, unless otherwise specified. In addition, the size, positional relationship, and the like of the components shown in the respective drawings may be exaggerated for clarity of explanation. Further, each of the elements constituting the present invention may be configured such that a plurality of elements are formed by the same part, and a plurality of elements are used as one part, or a function of realizing one part by a plurality of parts may be shared. In addition, the respective embodiments disclosed below can be applied in the same manner as long as there is no particular exclusion.

(實施的形態1) (Form 1 of implementation)

第1~3圖,是概念性地顯示本發明第一實施形態相關的半導體發光元件的構造。請參考第1~3圖,半導體發光元件主要具有由AlN(氮化鋁)構成的基板16、n型半導體層15、活性層13、p型半導體層12、正電極11與負電極14。在基板16的主表面上,形成有n型半導體層15。在n型半導體層15的局部表 面先形成有凸部,在此凸部上形成有活性層13。在活性層13上,形成有p型半導體層12。在p型半導體層12上,形成有正電極11。另外,在n型半導體層15的表面,在未形成上述凸部的區域則形成有負電極14。 Figs. 1 to 3 are conceptually showing the structure of a semiconductor light emitting element according to the first embodiment of the present invention. Referring to FIGS. 1 to 3, the semiconductor light-emitting device mainly has a substrate 16 made of AlN (aluminum nitride), an n-type semiconductor layer 15, an active layer 13, a p-type semiconductor layer 12, a positive electrode 11 and a negative electrode 14. On the main surface of the substrate 16, an n-type semiconductor layer 15 is formed. Partial table of the n-type semiconductor layer 15 A convex portion is formed on the surface, and an active layer 13 is formed on the convex portion. On the active layer 13, a p-type semiconductor layer 12 is formed. On the p-type semiconductor layer 12, a positive electrode 11 is formed. Further, on the surface of the n-type semiconductor layer 15, a negative electrode 14 is formed in a region where the above-described convex portion is not formed.

從作為發光層的活性層13發射的光的波長為350nm以下。在基板16,在位於與主表面為相反側的背面,形成有一週期凹凸構造21,週期凹凸構造21具有一週期L1,週期L1為從活性層13發射的光的波長除以構成基板16的氮化鋁的折射率與位於基板16的外部的外部介質的折射率的差之值(基準值)的1/3倍以上、5倍以下。 The wavelength of light emitted from the active layer 13 as the light-emitting layer is 350 nm or less. On the substrate 16, on the back surface on the opposite side to the main surface, a periodic concavo-convex structure 21 having a period L1 which is the wavelength of light emitted from the active layer 13 divided by the nitrogen constituting the substrate 16 is formed. The value of the difference between the refractive index of the aluminum and the refractive index of the external medium located outside the substrate 16 (reference value) is 1/3 times or more and 5 times or less.

以下,針對各元件作個別說明。 Hereinafter, each component will be individually described.

<基板> <Substrate>

作為基板16,可選用可在表面磊晶成長氮化物半導體結晶的基板、且滿足對半導體發光元件所發的光的波長區透光率高(例如此光的透光率50%以上)的基板。例如,作為基板16的材料,可列舉上述的AlN、甚至藍寶石、GaN等。 As the substrate 16, a substrate which can epitaxially grow a nitride semiconductor crystal on the surface and which has a high transmittance in a wavelength region of light emitted from the semiconductor light-emitting device (for example, a light transmittance of 50% or more) can be selected. . For example, examples of the material of the substrate 16 include the above-described AlN, and even sapphire, GaN, and the like.

基板16,如上所述在光取出面(背面)形成有週期凹凸構造21。具體而言,週期凹凸構造21含凸形狀部,此凸形狀部為如第2圖及第3圖所示的錐體形狀(例如具有底面的直徑D1、從底面到頂點的高度H1、側面與底面所成的角度θ的錐體形狀)。另外,凸部形狀亦可是如第4圖所示的半橢圓球形狀。 As described above, the substrate 16 has a periodic uneven structure 21 formed on the light extraction surface (back surface). Specifically, the periodic concavo-convex structure 21 includes a convex shape portion having a pyramid shape as shown in FIGS. 2 and 3 (for example, a diameter D1 having a bottom surface, a height H1 from a bottom surface to a vertex, and a side surface and The shape of the cone formed by the bottom surface θ). Further, the shape of the convex portion may be a semi-elliptical spherical shape as shown in Fig. 4 .

另外,週期凹凸構造的排列(凸形狀部的排列),只要是三角格子排列、正方格子排列、六方格子排列等週期排列方法即可,較好為填充因子(filling factor)為最大的三角格子排 列。還有,週期凹凸構造21,可具有其值為從半導體發光元件的發光波長除以構成基板16的氮化鋁的折射率與位於基板16的外部的外部介質的空氣的折射率的差之值(基準值)的1/3倍以上、5倍以下的週期L1。另外,週期凹凸構造21的高度H1,較好為相對於此週期L1的1/3倍以上、5倍以下的範圍。 In addition, the arrangement of the periodic concavo-convex structures (arrangement of the convex shape portions) may be a periodic arrangement method such as a triangular lattice arrangement, a square lattice arrangement, or a hexagonal lattice arrangement, and is preferably a triangular lattice row having a maximum filling factor (filling factor). Column. Further, the periodic concavo-convex structure 21 may have a value which is a value obtained by dividing the emission wavelength of the semiconductor light-emitting element by the difference between the refractive index of the aluminum nitride constituting the substrate 16 and the refractive index of the air of the external medium located outside the substrate 16. A period L1 of 1/3 times or more and 5 times or less (reference value). Further, the height H1 of the periodic concavo-convex structure 21 is preferably in the range of 1/3 times or more and 5 times or less with respect to the period L1.

另外,上述週期凹凸構造21的週期L1,更好為上述基準值的0.5倍以上、4倍以下,再更好為1倍以上、3倍以下。若是如此,可以更確實地提升光取出效率。另外,週期凹凸構造21的高度H1,相對於此週期L1較好為0.5倍以上、2倍以下,更好為0.6倍以上、1.8倍以下。若是如此,亦可以更確實地提升光取出效率。 In addition, the period L1 of the periodic concavo-convex structure 21 is preferably 0.5 times or more and 4 times or less of the above reference value, and more preferably 1 time or more and 3 times or less. If so, the light extraction efficiency can be improved more reliably. In addition, the height H1 of the periodic concavo-convex structure 21 is preferably 0.5 times or more and 2 times or less, more preferably 0.6 times or more and 1.8 times or less with respect to the period L1. If so, the light extraction efficiency can be improved more reliably.

接下來,針對週期凹凸構造21的製作方法,在以下敘述。週期凹凸構造21可藉由以下製程製作:第一、蝕刻罩幕製作步驟(第5圖的步驟(S41));第二、蝕刻步驟(第5圖的步驟(S42));第三、罩幕移除步驟(第5圖的步驟(S43))。蝕刻罩幕製作步驟是在基板16的背面上製作蝕刻罩幕圖形的步驟,可應用電子束微影法、光微影法、奈米壓印微影法等任意的方法。另外,為了提升在蝕刻步驟的蝕刻選擇比,藉由上述任意的方法形成具有圖形的罩幕圖形(例如為阻劑罩幕)後,沉積金屬而覆蓋此罩幕圖形,之後藉由舉離法與罩幕圖形一起移除此金屬的一部分,製作金屬的罩幕圖形亦可。 Next, a method of producing the periodic concavo-convex structure 21 will be described below. The periodic concavo-convex structure 21 can be fabricated by the following processes: first, etching mask making step (step (S41) of FIG. 5); second, etching step (step (S42) of FIG. 5); third, mask Screen removal step (step (S43) of Fig. 5). The etching mask manufacturing step is a step of forming an etching mask pattern on the back surface of the substrate 16, and any method such as an electron beam lithography method, a photolithography method, or a nanoimprint lithography method can be applied. In addition, in order to increase the etching selectivity ratio in the etching step, a patterned mask pattern (for example, a resist mask) is formed by any of the above methods, and the metal pattern is deposited to cover the mask pattern, and then lifted off. A part of the metal is removed together with the mask pattern to create a metal mask pattern.

以罩幕圖形作為蝕刻罩幕,蝕刻基板16的背面,在基板16的背面形成所欲的圖形。蝕刻的手法可以應用感應耦合電漿(ICP)蝕刻、反應性離子蝕刻(RIE)等的乾蝕刻、或是使 用酸性溶液或鹼性溶液作為蝕刻液的溼蝕刻等。在此處,為了形成週期性高的圖形,較好為應用乾蝕刻。在使用乾蝕刻的蝕刻步驟中,可使用阻劑等的樹脂材料、金屬等作為蝕刻罩幕,另外作為蝕刻氣體者,可應用氯系氣體、氟系氣體、溴系氣體等。還有,亦可使用在上述的蝕刻氣體混合氫、氧等的氣體。 The mask pattern is used as an etching mask to etch the back surface of the substrate 16, and a desired pattern is formed on the back surface of the substrate 16. The etching method can be performed by dry etching using inductively coupled plasma (ICP) etching, reactive ion etching (RIE), or the like. An acidic solution or an alkaline solution is used as a wet etching or the like of the etching solution. Here, in order to form a pattern having a high periodicity, dry etching is preferably applied. In the etching step using the dry etching, a resin material such as a resist or the like, a metal or the like can be used as the etching mask, and as the etching gas, a chlorine-based gas, a fluorine-based gas, a bromine-based gas or the like can be applied. Further, a gas such as hydrogen or oxygen may be mixed in the etching gas described above.

上述蝕刻步驟後,實施罩幕移除步驟。亦即,移除蝕刻罩幕的殘渣。蝕刻罩幕的殘渣的移除方法,藉由此蝕刻罩幕的材質作適當決定即可。例如,若蝕刻罩幕的材質是金屬,使用對此金屬具有溶解性的酸性溶液、鹼性溶液而除去殘渣即可。 After the above etching step, a mask removal step is performed. That is, the residue of the etching mask is removed. The method of removing the residue of the etching mask can be appropriately determined by etching the material of the mask. For example, if the material of the etching mask is metal, an acidic solution having a solubility in the metal or an alkaline solution may be used to remove the residue.

另外,在週期凹凸構造21之上,可形成樹脂或玻璃、石英等的密封材。進一步在密封材的表面,可形成凹凸構造。此凹凸構造的構成,可以與上述週期凹凸構造21為同樣的構成。 Further, on the periodic concavo-convex structure 21, a sealing material such as resin, glass, or quartz can be formed. Further, on the surface of the sealing material, a concavo-convex structure can be formed. The configuration of the uneven structure can be the same as that of the periodic uneven structure 21 described above.

<層積半導體層> <Laminated semiconductor layer>

層積半導體層是由III族氮化物半導體構成,如第1圖所示,是在基板16上依序層積n型半導體層15、活性層13及p型半導體層12而成。層積半導體層是以有機金屬化學氣相沉積法(MOCVD法)、有機金屬氣相磊晶法(MOVPE法)、分子束磊晶法(MBE法)、氫化物氣相磊晶法(HVPE法)等層積。 The laminated semiconductor layer is composed of a group III nitride semiconductor. As shown in FIG. 1, the n-type semiconductor layer 15, the active layer 13, and the p-type semiconductor layer 12 are sequentially laminated on the substrate 16. The laminated semiconductor layer is an organometallic chemical vapor deposition method (MOCVD method), an organometallic vapor phase epitaxy method (MOVPE method), a molecular beam epitaxy method (MBE method), a hydride vapor phase epitaxy method (HVPE method). ) Equal stacking.

n型半導體層: N-type semiconductor layer:

n型半導體層15較好是由AlxInyGaNz(x、y、z是滿足0<x≦1.0、0≦y≦0.1、0≦z<1.0的有理數且x+y+z=1.0)構成的半導體層,含n型不純物。作為不純物者,並未特別限定, 可列舉矽(Si)、鍺(Ge)、錫(Sn)等,較好可列舉Si、Ge。n型不純物的濃度可為1.0×1017/cm3以上、1.0×1020/cm3以下。另外,從n型半導體層15的結晶性及接觸特性的兩觀點,較好為:n型不純物的濃度為1.0×1018/cm3以上、1.0×1019/cm3以下。 The n-type semiconductor layer 15 is preferably made of Al x In y GaN z (x, y, z are rational numbers satisfying 0<x≦1.0, 0≦y≦0.1, 0≦z<1.0 and x+y+z=1.0 The semiconductor layer is composed of n-type impurities. The impurity is not particularly limited, and examples thereof include bismuth (Si), germanium (Ge), and tin (Sn). Preferred examples thereof include Si and Ge. The concentration of the n-type impurity may be 1.0 × 10 17 /cm 3 or more and 1.0 × 10 20 /cm 3 or less. Further, from the viewpoint of both the crystallinity and the contact property of the n-type semiconductor layer 15, the concentration of the n-type impurity is preferably 1.0 × 10 18 /cm 3 or more and 1.0 × 10 19 /cm 3 or less.

另外,n型半導體層15的膜厚為100nm以上、10000nm以下。另外,從n型半導體層15的結晶性及接觸特性的兩觀點,較好為:n型半導體層15的膜厚為500nm以上、3000nm以下。 Further, the thickness of the n-type semiconductor layer 15 is 100 nm or more and 10000 nm or less. Moreover, from the viewpoint of both the crystallinity and the contact property of the n-type semiconductor layer 15, the film thickness of the n-type semiconductor layer 15 is preferably 500 nm or more and 3,000 nm or less.

活性層: Active layer:

活性層13具有多重量子井構造。活性層13是由以下二層交互層積的層積構造構成:由AlxInyGaNz(x、y、z是滿足0<x≦1.0、0≦y≦0.1、0≦z<1.0的有理數且x+y+z=1.0)構成的井層;以及能隙能量較此井層的能隙能量大的由AlxInyGaNz(x、y、z是滿足0<x≦1.0、0≦y≦0.1、0≦z<1.0的有理數且x+y+z=1.0)構成的阻障層。井層的膜厚為1nm以上,較好為2nm以上。阻障層的膜厚為1nm以上,較好為2nm以上。 The active layer 13 has a multiple quantum well configuration. The active layer 13 is composed of a laminated structure of two layers of alternating layers: Al x In y GaN z (x, y, z are satisfying 0<x≦1.0, 0≦y≦0.1, 0≦z<1.0) a well layer composed of rational numbers and x+y+z=1.0); and Al x In y GaN z with energy gap energy greater than the energy gap energy of the well layer (x, y, z satisfy 0<x≦1.0, A barrier layer composed of 0≦y≦0.1, a rational number of 0≦z<1.0, and x+y+z=1.0). The film thickness of the well layer is 1 nm or more, preferably 2 nm or more. The film thickness of the barrier layer is 1 nm or more, preferably 2 nm or more.

p型半導體層: P-type semiconductor layer:

p型半導體層12是由例如p型披覆層及p型接觸層構成。p型披覆層是由AlxInyGaNz(x、y、z是滿足0<x≦1.0、0≦y≦0.1、0≦z<1.0的有理數且x+y+z=1.0)構成。由於有必要將電子封入活性層13,較好為p型披覆層的能隙能量大於構成活性層13的半導體層的能隙能量。因此,p型披覆層的Al成分,較好為大於構成活性層13的半導體層的Al成分。 The p-type semiconductor layer 12 is composed of, for example, a p-type cladding layer and a p-type contact layer. The p-type cladding layer is composed of Al x In y GaN z (x, y, z are rational numbers satisfying 0<x≦1.0, 0≦y≦0.1, 0≦z<1.0, and x+y+z=1.0). . Since it is necessary to encapsulate the electrons into the active layer 13, it is preferable that the energy gap energy of the p-type cladding layer is larger than the energy gap energy of the semiconductor layer constituting the active layer 13. Therefore, the Al component of the p-type cladding layer is preferably larger than the Al component of the semiconductor layer constituting the active layer 13.

作為p型披覆層的不純物者,可列舉適用的為鎂(Mg)。Mg的濃度(摻雜濃度)為1.0×1017/cm3以上,較好為1.0×1017/cm3以上。p型披覆層的膜厚為5nm以上、1000nm以下,較好為10nm以上、50nm以下。 As the impure substance of the p-type coating layer, magnesium (Mg) is preferably used. The concentration (doping concentration) of Mg is 1.0 × 10 17 /cm 3 or more, preferably 1.0 × 10 17 /cm 3 or more. The film thickness of the p-type cladding layer is 5 nm or more and 1000 nm or less, preferably 10 nm or more and 50 nm or less.

p型接觸層是由AlxInyGaNz(x、y、z是滿足0<x≦1.0、0≦y≦0.1、0≦z<1.0的有理數且x+y+z=1.0)構成。p型接觸層的Al成分較好為小於p型披覆層的Al成分。其理由是p型接觸層的能隙能量小於p型披覆層的能隙能量的情況,容易獲得良好的接觸特性。作為p型接觸層的不純物者,與p型披覆層同樣可列舉適用的為鎂(Mg)。Mg的摻雜濃度可為1.0×1017/cm3以上。p型接觸層的膜厚,從紫外光的穿透性與在p型接觸層的接觸特性的觀點,為1nm以上、50nm以下,較好為5nm以上、30nm以下。 The p-type contact layer is composed of Al x In y GaN z (x, y, and z are rational numbers satisfying 0<x≦1.0, 0≦y≦0.1, 0≦z<1.0, and x+y+z=1.0). The Al component of the p-type contact layer is preferably smaller than the Al component of the p-type cladding layer. The reason is that the energy gap energy of the p-type contact layer is smaller than that of the p-type cladding layer, and good contact characteristics are easily obtained. As the impurity of the p-type contact layer, as the p-type coating layer, magnesium (Mg) is preferably used. The doping concentration of Mg may be 1.0 × 10 17 /cm 3 or more. The film thickness of the p-type contact layer is from 1 nm to 50 nm, preferably from 5 nm to 30 nm, from the viewpoint of the transmittance of ultraviolet light and the contact property with the p-type contact layer.

<負電極層> <negative electrode layer>

負電極14是形成於n型半導體層15的曝露面(圍繞n型半導體層15的凸部的上表面)。n型半導體層15的曝露面是藉由局部移除(例如藉由蝕刻等移除)n型半導體層15的一部分及活性層13、p型半導體層12等而形成。作為蝕刻的手法者,可適用反應性離子蝕刻、感應耦合電漿蝕刻等的乾蝕刻。形成n型半導體層15的曝露面後,為了移除n型半導體層15中在被蝕刻面(曝露面)受到蝕刻造成的損傷的部分,較好為以酸性或鹼性溶液施以表面處理。其後,在上述n型半導體層15的曝露面形成具有歐姆特性的負電極14。 The negative electrode 14 is an exposed surface (the upper surface surrounding the convex portion of the n-type semiconductor layer 15) formed on the n-type semiconductor layer 15. The exposed surface of the n-type semiconductor layer 15 is formed by partially removing (for example, removing by etching or the like) a part of the n-type semiconductor layer 15 and the active layer 13, the p-type semiconductor layer 12, and the like. As the etching method, dry etching such as reactive ion etching or inductively coupled plasma etching can be applied. After the exposed surface of the n-type semiconductor layer 15 is formed, in order to remove the portion of the n-type semiconductor layer 15 which is damaged by etching on the surface to be etched (exposed surface), it is preferred to apply a surface treatment with an acidic or alkaline solution. Thereafter, a negative electrode 14 having an ohmic property is formed on the exposed surface of the n-type semiconductor layer 15.

負電極14、正電極11等的電極的圖形化,可使用 舉離法來實施。具體而言,在電極形成面塗佈光阻之後,藉由具備光罩的UV曝光機對光阻局部性地照射紫外線。其後,使光阻浸漬於顯影液,藉由使感光的光阻溶解而形成所需圖形的阻劑膜。使即將成為電極的金屬膜沉積於已被圖形化的阻劑膜上。然後,以剝離液溶解阻劑膜,並移除位於阻劑膜上的金屬膜,藉此使位於未形成阻劑膜的區域的金屬膜殘留,形成具有既定的圖形的金屬膜(電極)。 Patterning of the electrodes of the negative electrode 14, the positive electrode 11, etc., can be used Implement the law of separation. Specifically, after the photoresist is applied to the electrode forming surface, the photoresist is locally irradiated with ultraviolet rays by a UV exposure machine having a photomask. Thereafter, the photoresist is immersed in the developer to form a resist film of a desired pattern by dissolving the photosensitive photoresist. A metal film to be an electrode is deposited on the resist film that has been patterned. Then, the resist film is dissolved in a stripping solution, and the metal film on the resist film is removed, whereby the metal film in the region where the resist film is not formed remains, forming a metal film (electrode) having a predetermined pattern.

作為電極的圖形化的手法者,還可列舉以下的手法。亦即,在電極形成面(例如n型半導體層15的曝露面)形成即將成為電極的金屬膜。然後,在金屬膜上塗佈光阻後,經曝光、顯影步驟而將光阻圖形化。其後,以上述被圖形化的光阻(阻劑膜)為罩幕,以乾蝕刻或溼蝕刻局部地移除金屬膜。其後,以剝離液溶解光阻。如此,亦可形成電極。另外,上述舉離法與在金屬膜上形成阻劑圖形的圖形化手法比較,由於步驟簡略而較適用。 As the patterning method of the electrode, the following methods can also be cited. That is, a metal film to be an electrode is formed on the electrode forming surface (for example, the exposed surface of the n-type semiconductor layer 15). Then, after applying a photoresist on the metal film, the photoresist is patterned by exposure and development steps. Thereafter, the metal film is partially removed by dry etching or wet etching using the patterned photoresist (resist film) as a mask. Thereafter, the photoresist was dissolved in a stripping solution. In this way, an electrode can also be formed. Further, the above-described lift-off method is more suitable for the step of forming a resist pattern on the metal film because of the simple steps.

沉積構成負電極14的金屬膜的手法,可使用真空蒸鍍法、濺鍍法、化學氣相沉積法等任意的方法,但從排除金屬膜中的不純物的觀點,較好為使用真空蒸鍍法。用於負電極14的材料,可列舉各種材料而可從已知的材料選擇。沉積即將成為負電極14的金屬膜後,為了提升n型半導體層15與負電極14的接觸性,較好為以300℃以上、1100℃以下的溫度並以30秒以上、3分鐘以下的加熱時間的條件施以熱處理。針對熱處理的溫度及加熱時間,按照構成負電極14的金屬的種類以及金屬膜的膜厚以適當最佳的條件實施即可。 The method of depositing the metal film constituting the negative electrode 14 may be any method such as a vacuum deposition method, a sputtering method, or a chemical vapor deposition method. However, from the viewpoint of eliminating impurities in the metal film, vacuum evaporation is preferably used. law. The material used for the negative electrode 14 can be exemplified by various materials and can be selected from known materials. After depositing the metal film to be the negative electrode 14, in order to improve the contact between the n-type semiconductor layer 15 and the negative electrode 14, it is preferable to heat at a temperature of 300 ° C or more and 1100 ° C or less for 30 seconds or more and 3 minutes or less. The conditions of time are heat treated. The temperature and the heating time of the heat treatment may be carried out under appropriate optimum conditions depending on the type of the metal constituting the negative electrode 14 and the film thickness of the metal film.

<正電極層> <positive electrode layer>

正電極11,是形成於p型半導體層12中的p型接觸層上。正電極11的圖形化,較好為與負電極14的圖形化同樣使用舉離法。用於正電極11的材料,可列舉各種材料而可從已知的材料選擇。另外,由於正電極11較好為具有透光性,正電極11的厚度愈薄愈好。具體而言,正電極11的厚度為10nm以下、更適用為5nm以下。 The positive electrode 11 is formed on the p-type contact layer in the p-type semiconductor layer 12. For the patterning of the positive electrode 11, it is preferable to use the lift-off method in the same manner as the patterning of the negative electrode 14. The material used for the positive electrode 11 can be selected from various materials and can be selected from known materials. Further, since the positive electrode 11 is preferably light transmissive, the thinner the thickness of the positive electrode 11 is preferably. Specifically, the thickness of the positive electrode 11 is 10 nm or less, and more preferably 5 nm or less.

作為沉積即將成為正電極11的金屬膜的手法者,與負電極14的形成同樣可使用真空蒸鍍法、濺鍍法、化學氣相沉積法等任意的方法,但為了極力排除金屬膜中的不純物,較好為使用真空蒸鍍法。沉積即將成為正電極11的金屬膜後,為了提升與p型接觸層的接觸性,較好為以200℃以上、800℃以下的溫度並以30秒以上、3分鐘以下的時間施以熱處理。針對熱處理的溫度及時間,按照構成正電極11的金屬的種類以及正電極11的厚度選擇適當最佳的條件實施即可。 As a method of depositing a metal film to be the positive electrode 11, as in the formation of the negative electrode 14, any method such as a vacuum deposition method, a sputtering method, or a chemical vapor deposition method can be used, but in order to eliminate the metal film as much as possible. As the impurity, it is preferred to use a vacuum evaporation method. After the metal film to be the positive electrode 11 is deposited, in order to improve the contact with the p-type contact layer, it is preferred to apply heat treatment at a temperature of 200 ° C or higher and 800 ° C or lower for 30 seconds or longer and 3 minutes or shorter. The temperature and time of the heat treatment may be appropriately selected under the conditions of the type of the metal constituting the positive electrode 11 and the thickness of the positive electrode 11.

上述的半導體發光元件,是藉由如第5圖所示的製造步驟製造。亦即,請參考第5圖,首先實施基板準備步驟(S10)。在此步驟(S10)中,準備由AlN構成的基板。另外,在此階段尚未在基板的背面形成週期凹凸構造21。其次,實施半導體層形成步驟(S20)。在此步驟(S20)中,在基板16的主表面上,形成由p型半導體層12、活性層13、n型半導體層15構成的層積半導體層。這些p型半導體層12、活性層13、n型半導體層15分別如上述可藉由MOCVD法、MOVPE法等任意的方法形成。 The above semiconductor light emitting element is manufactured by the manufacturing process as shown in Fig. 5. That is, referring to Fig. 5, the substrate preparation step (S10) is first performed. In this step (S10), a substrate composed of AlN is prepared. Further, the periodic concavo-convex structure 21 has not been formed on the back surface of the substrate at this stage. Next, a semiconductor layer forming step (S20) is performed. In this step (S20), a laminated semiconductor layer composed of the p-type semiconductor layer 12, the active layer 13, and the n-type semiconductor layer 15 is formed on the main surface of the substrate 16. Each of the p-type semiconductor layer 12, the active layer 13, and the n-type semiconductor layer 15 can be formed by any method such as MOCVD method or MOVPE method as described above.

接下來,實施電極形成步驟(S30)。在此步驟中, 藉由蝕刻移除p型半導體層12、活性層13n型半導體層15的一部分,藉此如第1圖所示形成n型半導體層15的曝露面。另外,使用舉離法等,在p型半導體層12上形成正電極11、在n型半導體層15的曝露面上形成負電極14。 Next, an electrode forming step (S30) is performed. In this step, The p-type semiconductor layer 12 and a portion of the active layer 13n-type semiconductor layer 15 are removed by etching, whereby the exposed surface of the n-type semiconductor layer 15 is formed as shown in FIG. Further, the positive electrode 11 is formed on the p-type semiconductor layer 12 by the lift-off method or the like, and the negative electrode 14 is formed on the exposed surface of the n-type semiconductor layer 15.

之後,實施凹凸構造形成步驟(S40)。在此步驟(S40)中,首先實施罩幕形成步驟(S41)。在此步驟(S41)中,如上述使用微影法等在基板16的背面上形成蝕刻罩幕圖形。其次,實施蝕刻步驟(S42)。在此步驟(S42)中,對基板16的背面以上述蝕刻罩幕圖形為罩幕進行蝕刻。其結果,形成週期凹凸構造21。然後,下一步實施罩幕移除步驟(S43)。在此步驟(S43)中,藉由任意的方法移除蝕刻罩幕的殘渣。如此一來,可獲得示於第1圖的半導體發光元件。 Thereafter, a concavo-convex structure forming step (S40) is performed. In this step (S40), the mask forming step (S41) is first performed. In this step (S41), an etching mask pattern is formed on the back surface of the substrate 16 by lithography or the like as described above. Next, an etching step (S42) is performed. In this step (S42), the back surface of the substrate 16 is etched by using the above-described etching mask pattern as a mask. As a result, the periodic concavo-convex structure 21 is formed. Then, the mask removal step (S43) is carried out next. In this step (S43), the residue of the etching mask is removed by any method. In this way, the semiconductor light emitting element shown in Fig. 1 can be obtained.

(實施的形態2) (Form 2 of implementation)

本發明的實施的形態2相關的半導體發光元件,基板上具有與第1~3圖所示的半導體發光元件同樣的構造,但基板16的背面的構成則與第1~3圖所示的半導體發光元件不同。第6圖是概念性地顯示本發明的實施的形態2相關的半導體發光元件的基板16中的背面的平面構造。請參考第6圖,在本發明的實施的形態2中的半導體發光元件中,使用基板16的背面作為光取出面的一例,在此基板16的背面形成有週期凹凸構造21。然後,進一步在此週期凹凸構造21的表面形成有微細凹凸構造22。 In the semiconductor light-emitting device according to the second aspect of the present invention, the substrate has the same structure as the semiconductor light-emitting device shown in FIGS. 1 to 3, but the rear surface of the substrate 16 has the same structure as that of the first to third semiconductors. The light emitting elements are different. Fig. 6 is a plan view schematically showing the back surface of the substrate 16 of the semiconductor light-emitting device according to the second aspect of the present invention. Referring to Fig. 6, in the semiconductor light-emitting device of the second embodiment of the present invention, the back surface of the substrate 16 is used as an example of the light extraction surface, and the periodic uneven structure 21 is formed on the back surface of the substrate 16. Then, a fine uneven structure 22 is further formed on the surface of the periodic uneven structure 21.

亦即,示於第6圖的半導體發光元件,是具有含活性層13的半導體層,此活性層13是發光層,半導體發光元件的 表面包含作為光取出面的基板16的背面。在光取出面及半導體發光元件內折射率互異的二層的界面的至少任一個,形成有:週期凹凸構造21,具有比從活性層13發射的光的波長的0.5倍還大的週期L1;以及微細凹凸構造22,位於週期凹凸構造21的表面上,具有光的波長的0.5倍以下的平均直徑(直徑D2的平均值)。另外,平均直徑是分別測量以週期凹凸構造21的一週期為一邊的長度的正方形區域所含的微細凹凸構造22的直徑,而可藉由那些直徑的平均值決定。 That is, the semiconductor light emitting element shown in Fig. 6 is a semiconductor layer having an active layer 13 which is a light emitting layer and a semiconductor light emitting element. The surface includes the back surface of the substrate 16 as a light extraction surface. At least one of the interfaces of the two layers having different refractive indices in the light extraction surface and the semiconductor light emitting element is formed with a periodic uneven structure 21 having a period L1 larger than 0.5 times the wavelength of light emitted from the active layer 13 And the fine concavo-convex structure 22 is located on the surface of the periodic concavo-convex structure 21, and has an average diameter (average value of the diameter D2) of 0.5 times or less of the wavelength of light. Further, the average diameter is a diameter of the fine concavo-convex structure 22 included in the square region in which the length of one cycle of the periodic concavo-convex structure 21 is measured, and can be determined by the average value of those diameters.

另外,在此處使用基板16的背面作為光取出面的一例,而以在此基板16的背面16A形成週期凹凸構造21等為例來作說明,但形成上述週期凹凸構造21及微細凹凸構造22的場所不限於光取出面。亦即,形成週期凹凸構造21及微細凹凸構造22的場所只要在半導體發光元件內的折射率不同的層彼此的界面即可。例如在基板16的背面16A上形成密封材等的其他構件時的此背面16A與密封材(其他構件)的界面、或是亦可在半導體發光元件內的半導體層等折射率不同的層彼此的界面等,形成上述週期凹凸構造21及微細凹凸構造22。 In addition, the back surface of the substrate 16 is used as an example of the light extraction surface, and the periodic uneven structure 21 and the like are formed on the back surface 16A of the substrate 16 as an example. However, the periodic uneven structure 21 and the fine uneven structure 22 are formed. The location is not limited to the light extraction surface. In other words, the places where the periodic uneven structure 21 and the fine uneven structure 22 are formed may be any interface between layers having different refractive indices in the semiconductor light emitting element. For example, when another member such as a sealing material is formed on the back surface 16A of the substrate 16, the interface between the back surface 16A and the sealing material (other member) or the layer having a different refractive index such as a semiconductor layer in the semiconductor light emitting element may be used. The periodic uneven structure 21 and the fine uneven structure 22 are formed by an interface or the like.

另外,如果如上述在基板16的背面上形成密封材等的其他構件,此密封材表面(其他構件表面)就成為對於外部的光取出面。而且此時,除了折射率差最大的界面(例如此背面16A與密封材(其他構件)的界面)外,在密封材表面之成為光取出面的部分,亦可形成上述週期凹凸構造21與微細凹凸構造22。 Further, if another member such as a sealing material is formed on the back surface of the substrate 16 as described above, the surface of the sealing material (the surface of the other member) becomes a light extraction surface for the outside. Further, in this case, in addition to the interface having the largest difference in refractive index (for example, the interface between the back surface 16A and the sealing member (other member)), the periodic uneven structure 21 and the fine portion may be formed in the portion of the surface of the sealing material which becomes the light extraction surface. Concave structure 22.

本實施形態相關的半導體發光元件,p型半導體層 12、活性層13、n型半導體層15、正電極11、負電極14的構成基本上與第1~3圖所示的半導體發光元件同樣,另一方面,如上述,基板16的構成則與第1~3圖所示的半導體發光元件不同。因此,針對基板16的構成作說明。 Semiconductor light-emitting device according to the embodiment, p-type semiconductor layer 12. The structure of the active layer 13, the n-type semiconductor layer 15, the positive electrode 11, and the negative electrode 14 is basically the same as that of the semiconductor light-emitting elements shown in FIGS. 1 to 3, and the configuration of the substrate 16 is as described above. The semiconductor light-emitting elements shown in FIGS. 1 to 3 are different. Therefore, the configuration of the substrate 16 will be described.

<基板> <Substrate>

基板16的材質、特性等,基本上與第1~3圖所示的半導體發光元件中的基板16同樣,例如可使用藍寶石、AlN、GaN等。基板16,如上所述在光取出面(背面)具有週期凹凸構造21。具體而言,週期凹凸構造21含凸形狀部,此凸形狀部為如第6圖及第7圖所示的錐體形狀。另外,凸部形狀亦可是如第8圖所示的半橢圓球形狀。 The material, characteristics, and the like of the substrate 16 are basically the same as those of the substrate 16 in the semiconductor light-emitting device shown in FIGS. 1 to 3, and for example, sapphire, AlN, GaN, or the like can be used. The substrate 16 has a periodic concavo-convex structure 21 on the light extraction surface (back surface) as described above. Specifically, the periodic concavo-convex structure 21 includes a convex shaped portion which has a tapered shape as shown in FIGS. 6 and 7. Further, the shape of the convex portion may be a semi-elliptical spherical shape as shown in Fig. 8.

另外,週期凹凸構造21的排列,只要是三角格子排列、正方格子排列、六方格子排列等週期排列方法即可,較好為填充因子為最大的三角格子排列。還有,週期凹凸構造21,可具有相對於半導體發光元件的發光波長超過0.5倍的範圍的週期L1。另外,週期凹凸構造21的高度H1(凸形狀部的高度H1),較好為相對於週期L1的1/3倍以上、5倍的範圍。 Further, the arrangement of the periodic concavo-convex structures 21 may be a periodic arrangement method such as a triangular lattice arrangement, a square lattice arrangement, or a hexagonal lattice arrangement, and is preferably a triangular lattice arrangement in which the filling factor is the largest. Further, the periodic concavo-convex structure 21 may have a period L1 that is in a range of more than 0.5 times the emission wavelength of the semiconductor light emitting element. In addition, the height H1 of the periodic concavo-convex structure 21 (the height H1 of the convex shaped portion) is preferably in the range of 1/3 times or more and five times the period L1.

作為上述週期凹凸構造21的週期L1的數值範圍之例者,可例如為上述發光波長的2/3倍以上、1000倍以下,或是2倍以上、100倍以下。若是如此,可以更確實地提升光取出效率,同時可以抑制製造成本、可以獲得更均一的元件形狀與光輸出。另外,週期凹凸構造21的高度H1,相對於此週期L1較好為1/2倍以上、3倍以下,更好為3/4倍以上、2倍以下。若是如此,可以更確實地提升光取出效率,同時可以抑制製造成 本、可以獲得更均一的元件形狀與光輸出。 As an example of the numerical range of the period L1 of the periodic concavo-convex structure 21, for example, it may be 2/3 times or more and 1000 times or less, or 2 times or more and 100 times or less of the above-mentioned light emission wavelength. If so, the light extraction efficiency can be more surely improved, and at the same time, the manufacturing cost can be suppressed, and a more uniform element shape and light output can be obtained. In addition, the height H1 of the periodic concavo-convex structure 21 is preferably 1/2 times or more and 3 times or less, more preferably 3/4 times or more and 2 times or less with respect to the period L1. If so, the light extraction efficiency can be improved more surely, and the manufacturing can be suppressed. In this way, a more uniform component shape and light output can be obtained.

進一步,在形成有週期凹凸構造21的基板16的背面,在週期凹凸構造21的表面,形成比週期凹凸構造21小的微細凹凸構造22。微細凹凸構造22是配置在週期凹凸構造21的凸形狀部的表面與週期凹凸構造21的凹部(位於凸形狀部之間的平坦部)。微細凹凸構造22的平均直徑為半導體發光元件的發光波長的1/2以下,微細凹凸構造22的高度較好為平均直徑的0.1倍以上、10倍以下的範圍。另外,微細凹凸構造22的高度,更好為0.2倍以上、5倍以下,更好為0.5倍以上、2倍以下。微細凹凸構造22的微細凸形狀部,較好為具有錐體形狀或半橢圓球形狀。 Further, on the back surface of the substrate 16 on which the periodic concavo-convex structure 21 is formed, a fine concavo-convex structure 22 smaller than the periodic concavo-convex structure 21 is formed on the surface of the periodic concavo-convex structure 21. The fine concavo-convex structure 22 is a concave portion (a flat portion located between the convex portions) that is disposed on the surface of the convex portion of the periodic concavo-convex structure 21 and the periodic concavo-convex structure 21 . The average diameter of the fine concavo-convex structure 22 is 1/2 or less of the emission wavelength of the semiconductor light-emitting device, and the height of the fine concavo-convex structure 22 is preferably in the range of 0.1 times or more and 10 times or less of the average diameter. Further, the height of the fine concavo-convex structure 22 is preferably 0.2 times or more and 5 times or less, more preferably 0.5 times or more and 2 times or less. The fine convex portion of the fine concavo-convex structure 22 preferably has a pyramidal shape or a semi-elliptical spherical shape.

上述的微細凹凸構造22的平均直徑,更好為上述發光波長的1/30倍以上、2/5倍以下,再更好為1/10倍以上、3/10倍以下。若是如此,可以更確實地提升光取出效率。另外,微細凹凸構造22的平均高度,相對於此平均直徑較好為0.2倍以上、5倍以下,更好為0.5倍以上、2倍以下。若是如此,可以更確實地提升光取出效率。 The average diameter of the fine concavo-convex structure 22 is more preferably 1/30 times or more and 2/5 times or less, more preferably 1/10 times or more and 3/10 times or less. If so, the light extraction efficiency can be improved more reliably. In addition, the average height of the fine concavo-convex structure 22 is preferably 0.2 times or more and 5 times or less, more preferably 0.5 times or more and 2 times or less with respect to the average diameter. If so, the light extraction efficiency can be improved more reliably.

另外,微細凹凸構造22平均高度,是分別測量以週期凹凸構造的一週期為一邊的長度的正方形區域所含的微細凹凸構造的高度,而可藉由那些高度的平均值決定。 In addition, the average height of the fine concavo-convex structure 22 is a height of a fine concavo-convex structure included in a square region having a length of one cycle of the periodic concavo-convex structure, and can be determined by the average value of those heights.

其次,針對凹凸構造的製作方法在以下敘述。上述週期凹凸構造21與微細凹凸構造22,可藉由以下製程製作:第一、蝕刻罩幕製作步驟(第9圖的步驟(S410));第二、蝕刻步驟(第9圖的步驟(S420));第三、蝕刻罩幕移除步驟(第9圖的步 驟(S430))。蝕刻罩幕製作步驟是在基板製作蝕刻罩幕圖形的步驟,可應用電子束微影法、光微影法、奈米壓印微影法等。另外,為了提升在蝕刻步驟的蝕刻選擇比,亦可在藉由上述任意的方法形成具有圖形的罩幕圖形(例如阻劑罩幕)後,沉積金屬而覆蓋此罩幕圖形,其後藉由舉離法隨著罩幕圖形一併移除此金屬的一部分,藉此製作金屬的罩幕圖形。 Next, a method of producing the uneven structure will be described below. The periodic concavo-convex structure 21 and the fine concavo-convex structure 22 can be produced by the following processes: first, an etching mask making step (step (S410) of FIG. 9); second, etching step (step of FIG. 9 (S420) )); third, etching mask removal step (step of Figure 9) Step (S430)). The etching mask manufacturing step is a step of forming an etching mask pattern on the substrate, and an electron beam lithography method, a photo lithography method, a nanoimprint lithography method, or the like can be applied. In addition, in order to increase the etching selectivity ratio in the etching step, after forming a patterned mask pattern (for example, a resist mask) by any of the above methods, a metal is deposited to cover the mask pattern, and then The lift method removes a portion of the metal along with the mask pattern to create a metal mask pattern.

在此處,在微細凹凸構造22的形成,較好為以舉離法形成金屬的罩幕,更好為藉由鎳膜構成金屬的罩幕。其理由是,在蝕刻步驟(S420)被蝕刻的鎳粒子或鎳與蝕刻氣體的反應物再附著於基板16的背面,作用為奈米尺寸的蝕刻罩幕而可以確實地形成微細凹凸構造22。 Here, in the formation of the fine concavo-convex structure 22, it is preferable to form a mask for metal by lift-off method, and it is more preferable to form a mask for metal by a nickel film. The reason is that the nickel particles etched in the etching step (S420) or the reaction product of nickel and the etching gas adheres to the back surface of the substrate 16, and acts as a nano-sized etching mask to reliably form the fine uneven structure 22.

以罩幕圖形為蝕刻罩幕,蝕刻基板16的背面而在基板16的背面形成所欲的圖形。蝕刻的手法可以應用感應耦合電漿(ICP)蝕刻、反應性離子蝕刻(RIE)等的乾蝕刻、或是使用酸性溶液或鹼性溶液作為蝕刻液的溼蝕刻等。在此處,為了形成週期性高的圖形,較好為應用乾蝕刻。 The mask pattern is used as an etching mask to etch the back surface of the substrate 16 to form a desired pattern on the back surface of the substrate 16. The etching method may be dry etching using inductively coupled plasma (ICP) etching, reactive ion etching (RIE), or wet etching using an acidic solution or an alkaline solution as an etching solution. Here, in order to form a pattern having a high periodicity, dry etching is preferably applied.

在使用乾蝕刻的蝕刻步驟中,可使用阻劑等的樹脂材料、金屬等作為蝕刻罩幕。進一步,作為蝕刻氣體之反應氣體者,較好可應用氯系氣體、氟系氣體、溴系氣體等,另外亦可使用在的蝕刻氣體混合氫、氧、氬等的氣體。另外,為了形成微細凹凸構造22,較好為使用氟系氣體作為乾蝕刻氣體,特別是含碳的氟系氣體。 In the etching step using dry etching, a resin material such as a resist or the like, a metal or the like can be used as an etching mask. Further, as the reaction gas of the etching gas, a chlorine-based gas, a fluorine-based gas, a bromine-based gas, or the like is preferably used, and a gas such as hydrogen, oxygen, or argon may be mixed with the etching gas. Moreover, in order to form the fine uneven structure 22, it is preferable to use a fluorine-based gas as a dry etching gas, in particular, a fluorine-containing gas containing carbon.

或者,在上述罩幕製作步驟前,亦可藉由對基板16的背面作乾蝕刻、濕蝕刻等而預先予以粗面化。此時,在此 粗面上藉由上述製程形成週期凹凸構造21,可製作週期凹凸構造21與微細凹凸構造22的組合。 Alternatively, before the mask manufacturing step, the back surface of the substrate 16 may be roughened in advance by dry etching, wet etching, or the like. At this point, here The periodic uneven structure 21 is formed by the above-described process on the rough surface, and the combination of the periodic uneven structure 21 and the fine uneven structure 22 can be produced.

另外,亦可在形成週期凹凸構造21後,將金屬、陶瓷等的微粒子配置於基板16的背面(已形成有週期凹凸構造21的表面),以微粒子為蝕刻罩幕而施以乾蝕刻。這麼作亦可製作週期凹凸構造21與微細凹凸構造22的組合。上述微粒子的配置方法,可列舉將已溶解微粒子的溶劑塗佈於基板16的背面而予以乾燥的方法、在基板16的背面上形成金屬薄膜後再加熱而使金屬薄膜的金屬凝集的方法等,可使用任何的方法。 Further, after the periodic concavo-convex structure 21 is formed, fine particles such as metal or ceramic may be disposed on the back surface of the substrate 16 (the surface on which the periodic concavo-convex structure 21 is formed), and dry etching may be performed using the fine particles as an etching mask. In this way, a combination of the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 can be produced. The method of disposing the fine particles may be a method of applying a solvent in which fine particles are dissolved on the back surface of the substrate 16 and drying the film, and a method of forming a metal thin film on the back surface of the substrate 16 and then heating the metal thin film to agglomerate the metal thin film. Any method can be used.

如上所述,使週期凹凸構造21與微細凹凸構造22共存的製作方法有各式各樣,但考慮到製程的簡便性,最好是以含碳的氟系氣體蝕刻金屬罩幕的手法。 As described above, there are various methods for producing the periodic uneven structure 21 and the fine uneven structure 22. However, in view of the simplicity of the process, it is preferable to etch the metal mask with a fluorine-containing gas containing carbon.

蝕刻步驟後,移除蝕刻罩幕的殘渣作為罩幕移除步驟。針對蝕刻罩幕的殘渣的移除方法,可使用在實施的形態1所示的方法。 After the etching step, the residue of the etching mask is removed as a mask removal step. For the method of removing the residue of the etching mask, the method shown in the first embodiment can be used.

另外,在週期凹凸構造21與微細凹凸構造22的組合之上,可形成樹脂、玻璃、石英等的密封部。進一步在密封部的表面,可形成週期凹凸構造21與微細凹凸構造22的組合、或是週期凹凸構造21或微細凹凸構造22。 Further, on the combination of the periodic concavo-convex structure 21 and the fine concavo-convex structure 22, a sealing portion such as resin, glass, or quartz can be formed. Further, a combination of the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 or the periodic concavo-convex structure 21 or the fine concavo-convex structure 22 can be formed on the surface of the sealing portion.

上述本實施形態相關的半導體發光元件,是藉由如第9圖所述的製程來製造。亦即,請參考第9圖,實施基板準備步驟(S100)~電極形成步驟(S300)。這些步驟(S100)~(S300),基本上是可以與示於第5圖的步驟(S10)~(S30)同樣地實施。 The semiconductor light-emitting device according to the above-described embodiment is manufactured by the process described in FIG. That is, referring to Fig. 9, the substrate preparation step (S100) to the electrode formation step (S300) are carried out. These steps (S100) to (S300) can basically be carried out in the same manner as the steps (S10) to (S30) shown in Fig. 5.

之後,實施凹凸構造形成步驟(S400)。在此步驟 (S400)中,首先實施罩幕形成步驟(S410)。在此步驟(S410)中,如上述使用微影法等在基板16的背面上形成由金屬構成的蝕刻罩幕圖形。其次,實施蝕刻步驟(S420)。在此步驟(S420)中,對基板16的背面以上述蝕刻罩幕圖形為罩幕,藉由含碳的氟系氣體進行蝕刻。其結果,形成週期凹凸構造21及微細凹凸構造22。然後,下一步實施罩幕移除步驟(S430)。在此步驟(S430)中,藉由任意的方法移除蝕刻罩幕的殘渣。如此一來,可獲得示於第6圖的半導體發光元件。 Thereafter, a concave-convex structure forming step (S400) is performed. In this step (S400), first, a mask forming step (S410) is performed. In this step (S410), an etching mask pattern made of metal is formed on the back surface of the substrate 16 by lithography or the like as described above. Next, an etching step (S420) is performed. In this step (S420), the back surface of the substrate 16 is etched by the carbon-containing fluorine-based gas using the etching mask pattern as a mask. As a result, the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 are formed. Then, the mask removal step (S430) is carried out next. In this step (S430), the residue of the etching mask is removed by any method. In this way, the semiconductor light emitting element shown in Fig. 6 can be obtained.

另外,上述週期凹凸構造21及微細凹凸構造22,亦可不形成於基板16的背面,而形成在半導體發光元件內折射率不同的二層的界面。此時,亦會減低從發光層發射的光在此界面被反射.全反射的比例,結果可以提高半導體發光元件的光的取出效率。 Further, the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 may not be formed on the back surface of the substrate 16, but may form an interface of two layers having different refractive indices in the semiconductor light-emitting device. At this time, the light emitted from the luminescent layer is also reduced at this interface. The ratio of total reflection, as a result, can improve the light extraction efficiency of the semiconductor light emitting element.

在此處,列舉本發明的特徵性的構成,會有與上述的實施形態一部分重複的部分。 Here, the characteristic configuration of the present invention will be partially overlapped with the above-described embodiment.

亦即,本發明的一樣態,其特徵在於在半導體發光元件的表面(基板16的背面16A、或是在基板16的背面16A上配置密封材等的其他構件時則為此其他構件的表面等為光取出面的一例)、或半導體發光元件內的折射率不同的層彼此的界面(例如在基板16的背面16A上配置樹脂等的情況的背面16A與樹脂的界面、或是半導體發光元件內的半導體層等中折射率不同的層彼此的界面等),將具有超過發光波長的0.5倍的週期的週期凹凸構造21與具有相對於發光波長的1/2以下的平均直徑的微細凹凸構造22,一併形成在同一表面(或界面)上。 In other words, in the same state of the present invention, when the surface of the semiconductor light-emitting device (the back surface 16A of the substrate 16 or another member such as a sealing material is placed on the back surface 16A of the substrate 16), the surface of the other member is used. An interface between the layers of the light-receiving surface or the layers having different refractive indices in the semiconductor light-emitting device (for example, an interface between the back surface 16A and the resin when a resin or the like is placed on the back surface 16A of the substrate 16 or in the semiconductor light-emitting device) In the semiconductor layer or the like, the interface between the layers having different refractive indices, etc., the periodic uneven structure 21 having a period exceeding 0.5 times the emission wavelength and the fine uneven structure 22 having an average diameter of 1/2 or less with respect to the emission wavelength. , formed together on the same surface (or interface).

此時,由於在週期凹凸構造21彼此的間隙的平坦面部、週期凹凸構造21表面上等,形成有比週期凹凸構造小尺度的微細凹凸構造22,與週期凹凸構造21以單體存在的情況比較,可更緩和在表面.界面的折射率差而抑制反射、全反射等。 At this time, the fine uneven structure 22 having a smaller dimension than the periodic uneven structure is formed on the flat surface portion of the gap between the periodic uneven structures 21 and the surface of the periodic uneven structure 21, and the periodic uneven structure 21 is present as a single body. Can be more moderate on the surface. The refractive index difference of the interface suppresses reflection, total reflection, and the like.

另外,在週期凹凸構造21單體的情況,通常為了提高光取出效率,有必要形成在波長以下程度的小尺度的週期凹凸構造21;而在本實施樣態的構造中,即使是尺寸大於波長的週期凹凸構造21,藉由與微細凹凸構造22組合,仍可充分地提高光取出效率。也就是,即使發光波長為短波長,仍藉由降低花費於光取出構造的製作的成本、加上擴大製程範圍(process window),而容易製作均一的構造。 Further, in the case where the periodic concavo-convex structure 21 is single, in general, in order to improve the light extraction efficiency, it is necessary to form a small-scale periodic concavo-convex structure 21 having a wavelength or less; and in the configuration of the present embodiment, even if the size is larger than the wavelength By combining with the fine concavo-convex structure 22, the periodic concavo-convex structure 21 can sufficiently improve the light extraction efficiency. That is, even if the emission wavelength is a short wavelength, it is easy to produce a uniform structure by reducing the cost of fabrication of the light extraction structure and adding a process window.

還有,週期凹凸構造21的排列圖形較好為三角格子狀。 Further, the arrangement pattern of the periodic concavo-convex structure 21 is preferably a triangular lattice shape.

還有,週期凹凸構造21的形狀,較好為高折射率介質的剖面面積隨著從底部往頂點方向(光取出方向)前進而遞減。 Further, it is preferable that the shape of the periodic concavo-convex structure 21 is such that the cross-sectional area of the high refractive index medium decreases as it goes from the bottom to the vertex direction (light extraction direction).

還有,週期凹凸構造21的形狀為凸形狀,此凸形狀較好為錐體形狀或半橢圓球形狀。 Further, the shape of the periodic concavo-convex structure 21 is a convex shape, and the convex shape is preferably a pyramid shape or a semi-elliptical spherical shape.

本發明的一樣態具有以下的特徵,但並非將本發明限定為以下的樣態。 The same state of the present invention has the following features, but the present invention is not limited to the following aspects.

以具備具有n型III族氮化物半導體層(n型半導體層15)、III族氮化物半導體發光層(活性層13)及p型III族氮化物半導體層(p型半導體層12)的半導體層積構造為特徵。 A semiconductor layer having an n-type group III nitride semiconductor layer (n-type semiconductor layer 15), a group III nitride semiconductor light-emitting layer (active layer 13), and a p-type group III nitride semiconductor layer (p-type semiconductor layer 12) The product structure is characterized.

以具備具有覆晶構造、在從III族氮化物半導體發 光層到光取出面側對發光波長具有透明性的透明性基板(基板16)為特徵。 Having a flip chip structure and emitting from a group III nitride semiconductor The transparent layer (substrate 16) having transparency to the light emission wavelength from the light layer to the light extraction surface side is characterized.

以透明性基板為氮化鋁(AlN)基板或藍寶石基板為特徵。 The transparent substrate is characterized by an aluminum nitride (AlN) substrate or a sapphire substrate.

以發光波長為450nm以下或350nm以下為特徵。 It is characterized by an emission wavelength of 450 nm or less or 350 nm or less.

以週期凹凸構造21的高度為相對於週期的1/3~5倍的範圍、微細凹凸構造22的平均高度為相對於平均直徑的1/10~5倍的範圍為特徵。 The height of the periodic concavo-convex structure 21 is in the range of 1/3 to 5 times the period, and the average height of the fine concavo-convex structure 22 is in the range of 1/10 to 5 times the average diameter.

另外本發明的另一樣態的特徵在於:具備具有AlN基板(基板16)、n型III族氮化物半導體層(n型半導體層15)、III族氮化物半導體發光層(活性層13)及p型III族氮化物半導體層(p型半導體層12)的半導體層積構造,發光波長為350nm以下,在AlN基板表面上形成有具有相對於發光波長/(AlN基板的折射率與外部介質的折射率的差)的1/3~5倍的範圍的週期之週期凹凸構造21。 Further, another aspect of the present invention is characterized by comprising an AlN substrate (substrate 16), an n-type group III nitride semiconductor layer (n-type semiconductor layer 15), a group III nitride semiconductor light-emitting layer (active layer 13), and p The semiconductor layered structure of the group III nitride semiconductor layer (p-type semiconductor layer 12) has an emission wavelength of 350 nm or less, and is formed on the surface of the AlN substrate to have a refractive index with respect to the emission wavelength / (the refractive index of the AlN substrate and the external medium) The periodic uneven structure 21 of the period of the range of 1/3 to 5 times the difference in the rate.

還有,週期凹凸構造21的排列圖形較好為三角格子狀。 Further, the arrangement pattern of the periodic concavo-convex structure 21 is preferably a triangular lattice shape.

還有,週期凹凸構造21的形狀為凸形狀,此凸形狀較好為錐體形狀或半橢圓球形狀。 Further, the shape of the periodic concavo-convex structure 21 is a convex shape, and the convex shape is preferably a pyramid shape or a semi-elliptical spherical shape.

還有,週期凹凸構造21的高度,較好為相對於週期的1/3~5倍的範圍。 Further, the height of the periodic concavo-convex structure 21 is preferably in the range of 1/3 to 5 times the period.

另外,本發明的另一樣態的特徵在於其為上述半導體發光元件的製造方法,包含下列步驟:週期性地加工有機系薄膜;使用有機膜(有機系薄膜)形成金屬罩幕;使用罩幕藉 由乾蝕刻法,形成週期凹凸構造21。 Further, another aspect of the present invention is characterized in that it is a method of manufacturing the above semiconductor light-emitting element, comprising the steps of: periodically processing an organic film; forming an metal mask using an organic film (organic film); The periodic uneven structure 21 is formed by dry etching.

還有,以包含下列步驟為特徵:藉由使用金屬罩幕與氟系氣體的乾蝕刻法,同時形成週期凹凸構造21與微細凹凸構造22。 Further, the present invention is characterized in that the periodic uneven structure 21 and the fine uneven structure 22 are simultaneously formed by dry etching using a metal mask and a fluorine-based gas.

此時,藉由使用金屬罩幕與氟系氣體的乾蝕刻法,由於可人工式地均一.高純度地製作週期凹凸構造,加上藉由乾蝕刻後的以剝離金屬罩幕為目的的酸處理,在週期凹凸構造彼此的間隙的平坦面部、週期凹凸構造21表面等之上自發性第形成尺度遠小於波長的微細凹凸構造22,可以在一道製程同時形成週期凹凸構造21與微細凹凸構造22。藉此,可以均一.高精度地製作尺寸與波長同程度或大於波長、形狀的變化對特性賦予重大影響的週期凹凸構造21;且可以自發性地、綿密地形成尺度遠小於波長、形狀變化未對特性賦予太大影響的微細凹凸構造22。另外,以週期凹凸構造21與微細凹凸構造22是由相同材質構成為特徵。結果,提高加工形狀的均一性、製程的再現性,而可以在提高光取出效率與其均一性的同時,抑制製造成本在低水平。 At this time, by using a metal mask and a dry etching method of a fluorine-based gas, since it can be artificially uniform. The periodic uneven structure is produced in a high-purity manner, and the acid treatment for peeling off the metal mask by dry etching is performed, and the surface is formed on the flat surface of the gap between the periodic uneven structures and the surface of the periodic uneven structure 21, and the like. The fine concavo-convex structure 22 having a scale much smaller than the wavelength can simultaneously form the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 in one process. By this, you can be uniform. The periodic concavo-convex structure 21 having a size or wavelength equal to or greater than the wavelength and the shape change greatly affecting the characteristics is produced with high precision; and the scale can be spontaneously and densely formed to be much smaller than the wavelength, and the shape change does not greatly affect the characteristics. Fine concavo-convex structure 22. Further, the periodic concavo-convex structure 21 and the fine concavo-convex structure 22 are characterized by the same material. As a result, the uniformity of the processed shape and the reproducibility of the process can be improved, and the light extraction efficiency and the uniformity thereof can be improved, and the manufacturing cost can be suppressed to a low level.

根據本發明,藉由組合尺度不同的週期凹凸構造21與微細凹凸構造22,有效地抑制在基板表面(光取出面)、界面等的反射、全反射等。另外在可擴展製程範圍之下,發光波長即使是短波長,仍可以以高度的再現性、產量來製作可獲得高光取出效率與均一的光輸出的半導體發光元件。更進一步,在本岸明中,藉由同時製作週期凹凸構造21與微細凹凸構造22的製造方法,可以在提高加工形狀的均一性、製程的再現性且 提高光取出效率及其均一性的同時,抑制製造成本在低水平。 According to the present invention, by combining the periodic uneven structure 21 having different dimensions and the fine uneven structure 22, reflection, total reflection, and the like on the substrate surface (light extraction surface), the interface, and the like are effectively suppressed. Further, under the scalable process range, even if the emission wavelength is a short wavelength, a semiconductor light-emitting element capable of obtaining high light extraction efficiency and uniform light output can be produced with high reproducibility and throughput. Further, in the method of manufacturing the periodic concavo-convex structure 21 and the fine concavo-convex structure 22, it is possible to improve the uniformity of the processed shape and the reproducibility of the process. While improving the light extraction efficiency and its uniformity, the manufacturing cost is suppressed at a low level.

【實施例1】 [Example 1]

基於本發明的上述實施形態相關的半導體發光元件的構造,如第10圖及第11圖所示,製作實施例1相關的半導體發光元件。具體而言,在由單晶AlN構成的基板16上,藉由MOCVD法依序成長n型半導體層15、活性層13(發光層)、p型半導體層12而得到發光元件基板,在此發光元件基板,將正電極11及負電極14配置在既定的位置。含半導體發光元件的發光層的磊晶層,是以與上述實施的形態同樣的AlGaN系半導體構成,元件的發光波長為265nm。 According to the structure of the semiconductor light-emitting device according to the above-described embodiment of the present invention, as shown in FIGS. 10 and 11, a semiconductor light-emitting device according to the first embodiment is produced. Specifically, on the substrate 16 made of single crystal AlN, the n-type semiconductor layer 15, the active layer 13 (light-emitting layer), and the p-type semiconductor layer 12 are sequentially grown by MOCVD to obtain a light-emitting element substrate, and the light-emitting element substrate is obtained. In the element substrate, the positive electrode 11 and the negative electrode 14 are arranged at predetermined positions. The epitaxial layer of the light-emitting layer including the semiconductor light-emitting device is composed of the same AlGaN-based semiconductor as that of the above-described embodiment, and the light-emitting wavelength of the device is 265 nm.

在與已製作的半導體發光元件基板的磊晶層為相反側的基板面(光取出面),塗佈電子束阻劑,藉由以覆蓋半導體發光元件的發光部的方式作對準而作電子束描繪,製作蝕刻罩幕圖形。發光部是直徑100μm的圓形的區域,以發光部的中心為描繪中心,將描繪區域設為900μm×900μm。描繪圖形設為直徑220nm、圖形週期300nm,圖形排列設為三角格子排列。其次,在蝕刻罩幕圖形之上,藉由真空蒸鍍法沉積100nm~500nm的鎳。沉積鎳的理由如同在上述的實施的形態所說明,是為了提高基板16與蝕刻罩幕圖形的蝕刻選擇比。鎳的沉積後,將半導體發光元件基板浸漬於電子束阻劑的剝離液而移除阻劑及位於此阻劑上的鎳(舉離法)。這麼作,在基板16的背面上形成由鎳構成的罩幕圖形。 An electron beam resist is applied to a substrate surface (light extraction surface) on the opposite side of the epitaxial layer of the fabricated semiconductor light-emitting device substrate, and the electron beam is aligned by covering the light-emitting portion of the semiconductor light-emitting device. Depicting, making an etched mask pattern. The light-emitting portion is a circular region having a diameter of 100 μm, and the center of the light-emitting portion is the center of the drawing, and the drawing region is set to 900 μm × 900 μm. The drawing pattern was set to have a diameter of 220 nm and a pattern period of 300 nm, and the pattern arrangement was set to a triangular lattice arrangement. Next, on the etching mask pattern, nickel of 100 nm to 500 nm is deposited by vacuum evaporation. The reason for depositing nickel is as described in the above-described embodiment, in order to improve the etching selectivity of the substrate 16 and the etching mask pattern. After the deposition of nickel, the semiconductor light-emitting device substrate is immersed in the stripping liquid of the electron beam resist to remove the resist and the nickel on the resist (lifting method). In this manner, a mask pattern made of nickel is formed on the back surface of the substrate 16.

接下來,將上述半導體發光元件基板導入ICP蝕刻裝置,使用三氟甲烷(CHF3)氣體施以10分鐘~30分鐘的蝕刻處 理。其後,為了移除鎳的罩幕圖形,將半導體發光元件基板在20℃~30℃的鹽酸浸漬15分鐘。此時,為了防止半導體發光元件基板的電極金屬因鹽酸而腐蝕,在半導體發光元件基板的電極形成面預先塗佈光阻再使其硬化而作為保護膜使用。浸漬於鹽酸後,以超純水清洗半導體發光元件基板,再以剝離液溶解作為保護膜的光阻。 Next, the semiconductor light-emitting device substrate was introduced into an ICP etching apparatus, and an etching treatment was performed for 10 minutes to 30 minutes using a trifluoromethane (CHF 3 ) gas. Thereafter, in order to remove the mask pattern of nickel, the semiconductor light-emitting device substrate was immersed in hydrochloric acid at 20 ° C to 30 ° C for 15 minutes. In this case, in order to prevent the electrode metal of the semiconductor light-emitting device substrate from being corroded by hydrochloric acid, the electrode forming surface of the semiconductor light-emitting device substrate is coated with a photoresist and then cured to be used as a protective film. After immersing in hydrochloric acid, the semiconductor light-emitting device substrate was washed with ultrapure water, and the photoresist as a protective film was dissolved in a stripping solution.

藉此,製作具有圓錐底部的直徑250nm、週期L1為300nm、高度H1為250nm的錐體構造的基板16構成之實施例1的紫外發光的半導體發光元件。已製作的凹凸構造的掃描式電子顯微鏡照片示於第12圖及第13圖。 Thus, the ultraviolet light-emitting semiconductor light-emitting device of Example 1 having the funnel structure having a cone-shaped bottom portion having a diameter of 250 nm, a period L1 of 300 nm, and a height H1 of 250 nm was formed. Scanning electron micrographs of the produced concavo-convex structures are shown in Figs. 12 and 13.

準備在基板16形成凹凸構造前的紫外發光的半導體發光元件(比較例1)作為相對於實施例1的比較例。然後,針對這些實施例及比較例1的試樣,測定光輸出。將其結果示於第14圖。 A semiconductor light-emitting element (Comparative Example 1) of ultraviolet light emission before the formation of the uneven structure on the substrate 16 was prepared as a comparative example with respect to Example 1. Then, the light output was measured for the samples of these Examples and Comparative Example 1. The results are shown in Fig. 14.

請參考第14圖,橫軸是顯示以比較例1為基準的情況之實施例的光輸出比,縱軸是顯示試樣個數。以比較例1的光輸出為1.00時,實施例的光輸出比的平均值為1.31。第14圖是表示實施例1的試樣之紫外發光的半導體發光元件的光輸出比的直方圖。另外,實施例1的光輸出比的標準差為0.031,相當於光輸出比平均值的2.3%。亦即,實施例1的試樣,顯示其為發光輸出的變異程度極小的半導體發光元件。 Referring to Fig. 14, the horizontal axis represents the light output ratio of the embodiment in the case of Comparative Example 1, and the vertical axis represents the number of samples. When the light output of Comparative Example 1 was 1.00, the average value of the light output ratio of the Example was 1.31. Fig. 14 is a histogram showing the light output ratio of the ultraviolet light-emitting semiconductor light-emitting device of the sample of Example 1. Further, the standard deviation of the light output ratio of Example 1 was 0.031, which was equivalent to 2.3% of the average value of the light output ratio. That is, the sample of Example 1 showed a semiconductor light-emitting element having a very small variation in light-emitting output.

【實施例2】 [Example 2]

基於本發明的上述實施形態相關的半導體發光元件的構造,製作實施例2相關的半導體發光元件。另外,實施 例2相關的半導體發光元件的構成,基本上是與實施例1中的半導體發光元件同樣。亦即,在由單晶AlN構成的基板16上,藉由MOCVD法依序成長n型半導體層15、活性層13(發光層)、p型半導體層12而得到發光元件基板,在此發光元件基板,將正電極11及負電極14配置在既定的位置。含半導體發光元件的發光層的磊晶層,是以與上述實施的形態同樣的AlGaN系半導體構成,元件的發光波長為265nm。 A semiconductor light-emitting device according to Example 2 was produced based on the structure of the semiconductor light-emitting device according to the above-described embodiment of the present invention. In addition, implementation The configuration of the semiconductor light-emitting device of Example 2 is basically the same as that of the semiconductor light-emitting device of Example 1. In other words, on the substrate 16 made of single crystal AlN, the n-type semiconductor layer 15, the active layer 13 (light-emitting layer), and the p-type semiconductor layer 12 are sequentially grown by MOCVD to obtain a light-emitting element substrate. The substrate has the positive electrode 11 and the negative electrode 14 disposed at predetermined positions. The epitaxial layer of the light-emitting layer including the semiconductor light-emitting device is composed of the same AlGaN-based semiconductor as that of the above-described embodiment, and the light-emitting wavelength of the device is 265 nm.

在與已製作的半導體發光元件晶圓的發光元件層為相反側的基板面(光取出面),塗佈電子束阻劑,藉由以覆蓋半導體發光元件的發光部的方式作對準而作電子束描繪,製作蝕刻罩幕圖形。發光部是直徑100μm的圓區域,以發光部的中心為描繪中心,將描繪區域設為900μm×900μm。描繪圖形設為直徑300nm、圖形週期600nm,圖形排列設為正三角格子排列。其次,在罩幕圖形之上,藉由真空蒸鍍法沉積100nm~500nm的鎳。沉積鎳的理由與記載於實施例1的理由同樣。鎳的沉積後,將半導體發光元件基板浸漬於電子束阻劑的剝離液而移除阻劑及位於此阻劑上的鎳(舉離法)。這麼作,在基板16的背面上形成由鎳構成的罩幕圖形。 An electron beam resist is applied to a substrate surface (light extraction surface) on the opposite side of the light-emitting element layer of the fabricated semiconductor light-emitting device wafer, and is made electronic by aligning the light-emitting portion of the semiconductor light-emitting device The beam is drawn to create an etched mask pattern. The light-emitting portion is a circular region having a diameter of 100 μm, and the center of the light-emitting portion is the center of the drawing, and the drawing region is set to 900 μm × 900 μm. The drawing pattern was set to have a diameter of 300 nm and a pattern period of 600 nm, and the pattern arrangement was set to a regular triangular lattice arrangement. Next, on the mask pattern, nickel of 100 nm to 500 nm is deposited by vacuum evaporation. The reason for depositing nickel is the same as that described in the first embodiment. After the deposition of nickel, the semiconductor light-emitting device substrate is immersed in the stripping liquid of the electron beam resist to remove the resist and the nickel on the resist (lifting method). In this manner, a mask pattern made of nickel is formed on the back surface of the substrate 16.

接下來,將上述半導體發光元件基板導入ICp蝕刻裝置,使用三氟甲烷(CHF3)氣體施以30分鐘~80分鐘的蝕刻處理。藉由調整鎳膜厚與蝕刻時間,控制是否出現微細凹凸構造與形狀。最後,為了移除鎳的罩幕圖形,將半導體發光元件基板在已加熱至60℃~90℃的鹽酸浸漬15分鐘。此時,為了防止半導體發光元件基板的電極金屬因鹽酸而腐蝕,在半導體發光 元件基板的電極形成面預先塗佈光阻再使其硬化而作為保護膜使用。浸漬於鹽酸後,以超純水清洗,再以剝離液溶解作為保護膜的光阻。 Next, the semiconductor light-emitting device substrate was introduced into an ICp etching apparatus, and an etching treatment was performed for 30 minutes to 80 minutes using a trifluoromethane (CHF 3 ) gas. By adjusting the thickness of the nickel film and the etching time, it is controlled whether or not the fine concavo-convex structure and shape are formed. Finally, in order to remove the mask pattern of nickel, the semiconductor light-emitting device substrate was immersed in hydrochloric acid heated to 60 ° C to 90 ° C for 15 minutes. In this case, in order to prevent the electrode metal of the semiconductor light-emitting device substrate from being corroded by hydrochloric acid, the electrode forming surface of the semiconductor light-emitting device substrate is coated with a photoresist and then cured to be used as a protective film. After immersing in hydrochloric acid, it was washed with ultrapure water, and the photoresist as a protective film was dissolved in a stripping solution.

藉此,製作具有圓錐底部的直徑600nm、週期600nm、高度550nm的週期凹凸構造與平均直徑52nm、平均高度52nm的微細凹凸構造的基板構成之實施例2的紫外發光的半導體發光元件。已製作的凹凸構造的掃描式電子顯微鏡照片示於第15~17圖。如第17圖所示,上述微細凹凸構造在上述週期凹凸構造的凹部上分布得比在上述週期凹凸構造的凸部上還要密集。 Thus, an ultraviolet light-emitting semiconductor light-emitting device of Example 2 having a periodic concavity and convex structure having a diameter of 600 nm, a period of 600 nm, and a height of 550 nm and a fine concavo-convex structure having an average diameter of 52 nm and an average height of 52 nm was formed. Scanning electron micrographs of the produced concavo-convex structures are shown in Figures 15-17. As shown in Fig. 17, the fine concavo-convex structure is distributed more densely on the concave portion of the periodic concavo-convex structure than on the convex portion of the periodic concavo-convex structure.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件(比較例2)作為相對於實施例2的比較例。然後,針對這些實施例2及比較例2的試樣,測定光輸出。將其結果示於第18圖。 A semiconductor light-emitting element (Comparative Example 2) of ultraviolet light emission before the uneven structure was formed on the substrate was prepared as a comparative example with respect to Example 2. Then, the light output was measured for the samples of Example 2 and Comparative Example 2. The results are shown in Fig. 18.

請參考第18圖,橫軸是顯示以比較例2為基準的情況之實施例2的光輸出比,縱軸是顯示試樣個數。以比較例2的光輸出為1.00時,實施例2的光輸出比的平均值為1.70。另外,若將僅具有微細凹凸構造的紫外發光的半導體發光元件作為比較例3,比較例3相對於比較例2的光輸出比的平均值為1.25。其結果,可顯示以實施例2製作的具有週期凹凸構造與微細凹凸構造二者的構造的優位性。第18圖是表示實施例2的試樣之紫外發光的半導體發光元件的光輸出比的直方圖。另外,實施例2的光輸出比的標準差為0.029,相當於實施例2的光輸出比平均值的1.7%。亦即,實施例2的試樣,亦顯示其為 發光輸出的變異程度極小的半導體發光元件。 Referring to Fig. 18, the horizontal axis represents the light output ratio of the second embodiment in the case of Comparative Example 2, and the vertical axis represents the number of samples. When the light output of Comparative Example 2 was 1.00, the average value of the light output ratio of Example 2 was 1.70. In addition, when the ultraviolet light-emitting semiconductor light-emitting device having only the fine uneven structure was used as Comparative Example 3, the average value of the light output ratio of Comparative Example 3 with respect to Comparative Example 2 was 1.25. As a result, the superiority of the structure having both the periodic uneven structure and the fine uneven structure produced in Example 2 can be exhibited. Fig. 18 is a histogram showing the light output ratio of the ultraviolet light-emitting semiconductor light-emitting device of the sample of Example 2. Further, the standard deviation of the light output ratio of Example 2 was 0.029, which corresponded to 1.7% of the average value of the light output ratio of Example 2. That is, the sample of Example 2 is also shown to be A semiconductor light-emitting element having a very small variation in light-emitting output.

【實施例3】 [Example 3]

為了確認形成於根據本發明的半導體發光元件的週期凹凸構造21的功效,進行如以下的模擬計算。亦即,計算以作為發光層的AlGaN層發出的光(波長265nm)經由AlN基板與在AlN基板表面加工而得的週期凹凸構造(由AlN構成的圓錐的二次元週期排列(三角格子))而取出到外界(空氣)的光取出效率。另外,亦計算在同樣的系統在無週期凹凸構造的情況的光取出效率。 In order to confirm the efficacy of the periodic uneven structure 21 formed in the semiconductor light emitting element according to the present invention, the following simulation calculation was performed. In other words, the light emitted from the AlGaN layer as the light-emitting layer (wavelength: 265 nm) is calculated by the AlN substrate and the periodic uneven structure (the secondary element period arrangement (triangular lattice) of the cone made of AlN) processed on the surface of the AlN substrate. The light extraction efficiency of the outside (air) is taken out. In addition, the light extraction efficiency in the case where the same system has no periodic uneven structure is also calculated.

計算是使用時域有限差分法(FDTD法),設定偶極點光源作為初期光源,但藉由複數次改變偶極的震動方向、位置等而作計算、平均化(擬無序化),以人工方式再現非同調的光源。折射率則針對AlGaN部假定為2.43、AlN部假定為2.29、空氣部假定為1.0。針對從發光層觀察而為與光取出面的相反側(背面側),由於通常光藉由p-GaN層而被吸收,作為吸收邊界。將其結果示於第19圖及第20圖。 The calculation uses the finite difference time domain method (FDTD method) to set the dipole point source as the initial source, but calculates and averages (quasi-disordered) by artificially changing the direction and position of the dipole. The way to reproduce a non-coherent light source. The refractive index is assumed to be 2.43 for the AlGaN portion, 2.29 for the AlN portion, and 1.0 for the air portion. The opposite side (back side) from the light extraction surface as viewed from the light-emitting layer is normally absorbed by the p-GaN layer as an absorption boundary. The results are shown in Fig. 19 and Fig. 20.

第19圖及第20圖,是計算以作為發光層的AlGaN層發出的光(波長265nm)經由AlN基板與在AlN基板表面加工而得的週期凹凸構造(由AlN構成的圓錐的二次元週期排列(三角格子))而取出到外界(空氣)的光取出效率,將其以無週期凹凸構造的情況(平面)的結果歸一化後的數值(光輸出比)作顯示。週期凹凸構造的凸形狀部(圓錐形狀部)的底部的寬度與週期設為一致。第19圖的橫軸顯示週期凹凸構造的週期(單位:nm),縱軸顯示光輸出比。在第19圖中,顯示高寬比不同的每 個情況的數據。另外,第20圖的橫軸顯示高寬比(週期凹凸構造的凸形狀部(圓錐形狀部)的底部的高度對比於凸形狀部的寬度的比值),縱軸顯示光輸出比。在第20圖中,顯示週期凹凸構造的每個週期(a)的數據。 19 and 20 are diagrams for calculating a periodic concavo-convex structure (a quadratic periodic arrangement of a cone made of AlN) which is formed by processing an AlGaN substrate and a surface of an AlN substrate by light emitted from an AlGaN layer as a light-emitting layer (wavelength: 265 nm). (Triangular lattice)) The light extraction efficiency of the outside (air) is taken out, and the numerical value (light output ratio) normalized by the result of the case (planar) without the periodic uneven structure is displayed. The width of the bottom of the convex portion (conical portion) of the periodic uneven structure is set to coincide with the period. The horizontal axis of Fig. 19 shows the period (unit: nm) of the periodic uneven structure, and the vertical axis shows the light output ratio. In Figure 19, each aspect with a different aspect ratio is displayed. Data for a situation. Further, the horizontal axis of Fig. 20 shows the aspect ratio (the ratio of the height of the bottom portion of the convex portion (conical portion) of the periodic concavo-convex structure to the width of the convex portion), and the vertical axis indicates the light output ratio. In Fig. 20, data of each period (a) of the periodic uneven structure is shown.

請參考第19圖,在週期為200nm~450nm的範圍中,高寬比1.0的情況光輸出比成為最大。另外,請參考第20圖,高寬比1.0的情況光輸出比成為最大。 Referring to Fig. 19, in the range of 200 nm to 450 nm, the light output ratio becomes maximum when the aspect ratio is 1.0. In addition, please refer to Fig. 20, and the light output ratio becomes maximum when the aspect ratio is 1.0.

另外第19圖及第20圖是以二次元的計算的結果,但是確認是得到與以三次元的計算幾乎同樣的傾向的結果。 In addition, the 19th and 20th figures are the results of the calculation of the binary element, but it is confirmed that the result is almost the same as the calculation of the three-dimensional element.

【實施例4】 [Embodiment 4]

為了確認形成於根據本發明的半導體發光元件的週期凹凸構造21的功效,進行如以下的模擬計算。亦即,計算以作為發光層的AlGaN層發出的光(波長265nm)經由AlN基板與在AlN基板表面加工而得的週期凹凸構造(由AlN構成的圓錐的二次元週期排列(三角格子))而取出到外界(密封材層)的光取出效率。另外,亦計算在同樣的系統在無週期凹凸構造的情況的光取出效率。另外,計算方法與實施例3同樣。折射率則針對AlGaN部假定為2.43、AlN部假定為2.29、密封材部假定為1.45。作為密封材部者,是設定SiO2、樹脂等。而其他的條件設為與實施例3同樣。 In order to confirm the efficacy of the periodic uneven structure 21 formed in the semiconductor light emitting element according to the present invention, the following simulation calculation was performed. In other words, the light emitted from the AlGaN layer as the light-emitting layer (wavelength: 265 nm) is calculated by the AlN substrate and the periodic uneven structure (the secondary element period arrangement (triangular lattice) of the cone made of AlN) processed on the surface of the AlN substrate. The light extraction efficiency of the outside (sealing material layer) is taken out. In addition, the light extraction efficiency in the case where the same system has no periodic uneven structure is also calculated. In addition, the calculation method is the same as that of the third embodiment. The refractive index is assumed to be 2.43 for the AlGaN portion, 2.29 for the AlN portion, and 1.45 for the sealing material portion. As the sealing material portion, SiO 2 , a resin, or the like is set. The other conditions were the same as in the third embodiment.

第21圖及第22圖,是計算以AlGaN層發出的光(波長265nm)經由AlN基板與在AlN基板表面加工而得的週期凹凸構造(由AlN構成的圓錐的二次元週期排列(三角格子))而取出到外界(密封材層)的光取出效率,將其以在AlN基板表面無週 期凹凸構造的情況的平面取出到外界(空氣層)的情況的光取出率的計算結果歸一化後的數值(光輸出比)作顯示。 21 and 22 are diagrams for calculating a periodic concavo-convex structure (a quadratic lattice arrangement of a cone made of AlN) by processing an AlGaN substrate and a surface of an AlN substrate by a light emitted from an AlGaN layer (wavelength: 265 nm). ) and the light extraction efficiency of the outside (sealing material layer) is taken out, and there is no circumference on the surface of the AlN substrate. In the case where the plane of the period of the uneven structure is taken out to the outside (air layer), the normalized value (light output ratio) of the calculation result of the light extraction rate is displayed.

第21圖的橫軸顯示週期凹凸構造的週期(單位:nm),縱軸顯示光輸出比。在第21圖中,顯示高寬比不同的每個情況的數據。另外,第22圖的橫軸顯示高寬比,縱軸顯示光輸出比。在第22圖中,顯示週期凹凸構造的每個週期(a)的數據。 The horizontal axis of Fig. 21 shows the period (unit: nm) of the periodic uneven structure, and the vertical axis shows the light output ratio. In Fig. 21, data of each case in which the aspect ratio is different is displayed. In addition, the horizontal axis of Fig. 22 shows the aspect ratio, and the vertical axis shows the light output ratio. In Fig. 22, the data of each period (a) of the periodic uneven structure is shown.

根據實施例3及實施例4的結果,瞭解到即使是例如相同基板、波長、週期凹凸構造,根據密封構件等的外部介質的折射率,最佳的光取出構造則不同。不過,從AlN基板與在AlN基板表面加工而得的週期凹凸構造的光的取出,無論是取出到空氣或密封材層的情況,均對生產步驟有益,根據這些結果,可確認週期凹凸構造21的功效。 According to the results of the third embodiment and the fourth embodiment, it is understood that the optimum light extraction structure differs depending on the refractive index of the external medium such as the sealing member even in the case of, for example, the same substrate, wavelength, and periodic uneven structure. However, the extraction of light from the AlN substrate and the periodic concavo-convex structure processed on the surface of the AlN substrate is advantageous for the production step in the case of taking out the air or the sealing material layer, and based on these results, the periodic uneven structure 21 can be confirmed. The effect.

【實施例5】 [Embodiment 5]

基於本發明的上述實施形態相關的半導體發光元件的構造,製作實施例5相關的半導體發光元件。另外,實施例5相關的半導體發光元件的構成,基本上與實施例1中的半導體發光元件同樣。含半導體發光元件的發光層的磊晶層,是以與上述實施的形態同樣的AlGaN系半導體構成,元件的發光波長為265nm。 A semiconductor light-emitting device according to Example 5 was produced based on the structure of the semiconductor light-emitting device according to the above-described embodiment of the present invention. Further, the configuration of the semiconductor light-emitting device of the fifth embodiment is basically the same as that of the semiconductor light-emitting device of the first embodiment. The epitaxial layer of the light-emitting layer including the semiconductor light-emitting device is composed of the same AlGaN-based semiconductor as that of the above-described embodiment, and the light-emitting wavelength of the device is 265 nm.

在與已製作的半導體發光元件晶圓的發光元件層為相反的基板面(光取出面),塗佈電子束阻劑,藉由以覆蓋半導體發光元件的發光部的方式作對準而作電子束描繪,製作蝕刻罩幕圖形。發光部是直徑100μm的圓區域,以發光部的中心為描繪中心,將描繪區域設為900μm×900μm。描繪圖形設為直 徑180nm、圖形週期300nm,圖形排列設正為三角格子排列。其次,在罩幕圖形之上,藉由真空蒸鍍法沉積100nm~500nm的鎳。沉積鎳的理由與記載於實施例1的理由同樣。鎳的沉積後,將半導體發光元件基板浸漬於電子束阻劑的剝離液而移除阻劑及位於此阻劑上的鎳(舉離法)。這麼作,在基板16的背面上形成由鎳構成的罩幕圖形。 Applying an electron beam resist to a substrate surface (light extraction surface) opposite to the light-emitting element layer of the fabricated semiconductor light-emitting device wafer, and aligning the light-emitting portion of the semiconductor light-emitting device to form an electron beam Depicting, making an etched mask pattern. The light-emitting portion is a circular region having a diameter of 100 μm, and the center of the light-emitting portion is the center of the drawing, and the drawing region is set to 900 μm × 900 μm. The drawing is set to straight The diameter is 180 nm, the pattern period is 300 nm, and the pattern arrangement is set to a triangular lattice arrangement. Next, on the mask pattern, nickel of 100 nm to 500 nm is deposited by vacuum evaporation. The reason for depositing nickel is the same as that described in the first embodiment. After the deposition of nickel, the semiconductor light-emitting device substrate is immersed in the stripping liquid of the electron beam resist to remove the resist and the nickel on the resist (lifting method). In this manner, a mask pattern made of nickel is formed on the back surface of the substrate 16.

接下來,與實施例2同樣,將上述半導體發光元件基板導入ICP蝕刻裝置,使用三氟甲烷(CHF3)氣體施以10分鐘~80分鐘的蝕刻處理。如實施例5與實施例2比較,圖形尺寸較小的構造則蝕刻處理時間相對變短。最後,為了移除鎳的罩幕圖形,將半導體發光元件基板在已加熱至60℃~90℃的鹽酸浸漬15分鐘。另外,藉由調整鹽酸的溫度,可控制是否出現微細凹凸構造與形狀。另外,與實施例2的情況同樣,為了防止半導體發光元件基板的電極金屬因鹽酸而腐蝕,在半導體發光元件基板的電極形成面預先塗佈光阻再使其硬化而作為保護膜使用。浸漬於鹽酸後,以超純水清洗,再以剝離液溶解作為保護膜的光阻。 Next, in the same manner as in Example 2, the semiconductor light-emitting device substrate was introduced into an ICP etching apparatus, and an etching treatment was performed for 10 minutes to 80 minutes using a trifluoromethane (CHF 3 ) gas. As in the case of the embodiment 5 and the embodiment 2, the etching process time is relatively short. Finally, in order to remove the mask pattern of nickel, the semiconductor light-emitting device substrate was immersed in hydrochloric acid heated to 60 ° C to 90 ° C for 15 minutes. Further, by adjusting the temperature of the hydrochloric acid, it is possible to control whether or not a fine uneven structure and shape are formed. In the same manner as in the case of the second embodiment, in order to prevent the electrode metal of the semiconductor light-emitting device substrate from being corroded by hydrochloric acid, the electrode forming surface of the semiconductor light-emitting device substrate is coated with a photoresist and then cured to be used as a protective film. After immersing in hydrochloric acid, it was washed with ultrapure water, and the photoresist as a protective film was dissolved in a stripping solution.

藉此,製作具有圓錐底部的直徑300nm、週期300nm、高寬比為1的週期凹凸構造與平均直徑33nm、平均高度33nm的微細凹凸構造的基板構成之實施例5的紫外發光的半導體發光元件。 Thus, an ultraviolet light-emitting semiconductor light-emitting device of Example 5 having a periodic concavo-convex structure having a diameter of 300 nm, a period of 300 nm, and an aspect ratio of 1, and a fine concavo-convex structure having an average diameter of 33 nm and an average height of 33 nm was prepared.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件,作為相對於實施例5的比較例,而為比較例4。然後,針對這些實施例5及比較例4的試樣,測定光輸出。將其結果示 於第23圖。 The ultraviolet light-emitting semiconductor light-emitting device before the formation of the uneven structure on the substrate was prepared as Comparative Example 4 as a comparative example with respect to Example 5. Then, the light output was measured for the samples of Example 5 and Comparative Example 4. Show the results In Figure 23.

請參考第23圖,橫軸是顯示以比較例4為基準的情況之實施例5的光輸出比,縱軸是顯示試樣個數。以比較例4的光輸出為1.00時,實施例5的光輸出比的平均值為1.96。如從第23圖所瞭解,在實施例5獲得高光輸出比,可顯示具有週期凹凸構造與微細凹凸構造二者的構造的優位性。另外,實施例5的光輸出比的標準差為0.07,相當於光輸出比平均值的3.6%。如此,實施例5的試樣亦顯示其為發光輸出的變異程度相對較小的半導體發光元件。 Referring to Fig. 23, the horizontal axis represents the light output ratio of Example 5 in the case of Comparative Example 4, and the vertical axis represents the number of samples. When the light output of Comparative Example 4 was 1.00, the average value of the light output ratio of Example 5 was 1.96. As understood from Fig. 23, the high light output ratio obtained in Example 5 can show the superiority of the structure having both the periodic uneven structure and the fine uneven structure. Further, the standard deviation of the light output ratio of Example 5 was 0.07, which corresponds to 3.6% of the average value of the light output ratio. Thus, the sample of Example 5 also showed that it was a semiconductor light-emitting element having a relatively small degree of variation in light-emitting output.

【實施例6】 [Embodiment 6]

基於本發明的上述實施形態相關的半導體發光元件的構造,製作實施例6相關的半導體發光元件。另外,實施例6相關的半導體發光元件的構成,基本上與實施例1中的半導體發光元件同樣。另外,含半導體發光元件的發光層的磊晶層的材料與元件的發光波長是與上述的實施例5同樣。 A semiconductor light-emitting device according to Example 6 was produced based on the structure of the semiconductor light-emitting device according to the above-described embodiment of the present invention. Further, the configuration of the semiconductor light-emitting device of the sixth embodiment is basically the same as that of the semiconductor light-emitting device of the first embodiment. Further, the material of the epitaxial layer of the light-emitting layer including the semiconductor light-emitting element and the light-emitting wavelength of the element were the same as those of the above-described fifth embodiment.

在與已製作的半導體發光元件晶圓的發光元件層為相反的基板面(光取出面),與實施例5同樣藉由電子束描繪,製作蝕刻罩幕圖形。發光部是直徑100μm的圓區域,以發光部的中心為描繪中心,將描繪區域設為900μm×900μm。描繪圖形設為直徑200nm、圖形週期400nm,圖形排列設為正三角格子排列。其次,與實施例5同樣,在罩幕圖形之上,藉由真空蒸鍍法沉積100nm~500nm的鎳。鎳的沉積後,將半導體發光元件基板浸漬於電子束阻劑的剝離液而移除阻劑及位於此阻劑上的鎳(舉離法)。這麼作,在基板16的背面上形成由鎳構成的罩 幕圖形。 An etching mask pattern was produced by electron beam drawing in the same manner as in Example 5 on the substrate surface (light extraction surface) opposite to the light-emitting element layer of the fabricated semiconductor light-emitting device wafer. The light-emitting portion is a circular region having a diameter of 100 μm, and the center of the light-emitting portion is the center of the drawing, and the drawing region is set to 900 μm × 900 μm. The drawing pattern was set to have a diameter of 200 nm and a pattern period of 400 nm, and the pattern arrangement was set to a regular triangular lattice arrangement. Next, in the same manner as in Example 5, nickel of 100 nm to 500 nm was deposited by vacuum evaporation on the mask pattern. After the deposition of nickel, the semiconductor light-emitting device substrate is immersed in the stripping liquid of the electron beam resist to remove the resist and the nickel on the resist (lifting method). In this way, a cover made of nickel is formed on the back surface of the substrate 16. Curtain graphics.

接下來,與實施例2同樣,將上述半導體發光元件基板導入ICP蝕刻裝置,使用三氟甲烷(CHF3)氣體施以10分鐘~80分鐘的蝕刻處理。最後,為了移除鎳的罩幕圖形,將半導體發光元件基板在已加熱至60℃~90℃的鹽酸浸漬15分鐘。另外,與實施例2的情況同樣,為了防止半導體發光元件基板的電極金屬因鹽酸而腐蝕,在半導體發光元件基板的電極形成面預先塗佈光阻再使其硬化而作為保護膜使用。浸漬於鹽酸後,以超純水清洗,再以剝離液溶解作為保護膜的光阻。 Next, in the same manner as in Example 2, the semiconductor light-emitting device substrate was introduced into an ICP etching apparatus, and an etching treatment was performed for 10 minutes to 80 minutes using a trifluoromethane (CHF 3 ) gas. Finally, in order to remove the mask pattern of nickel, the semiconductor light-emitting device substrate was immersed in hydrochloric acid heated to 60 ° C to 90 ° C for 15 minutes. In the same manner as in the case of the second embodiment, in order to prevent the electrode metal of the semiconductor light-emitting device substrate from being corroded by hydrochloric acid, the electrode forming surface of the semiconductor light-emitting device substrate is coated with a photoresist and then cured to be used as a protective film. After immersing in hydrochloric acid, it was washed with ultrapure water, and the photoresist as a protective film was dissolved in a stripping solution.

藉此,製作具有圓錐底部的直徑400nm、週期400nm、高寬比為1的週期凹凸構造與平均直徑33nm、平均高度33nm的微細凹凸構造的基板構成之實施例6的紫外發光的半導體發光元件。 Thus, an ultraviolet light-emitting semiconductor light-emitting device of Example 6 having a periodic concave-convex structure having a diameter of 400 nm, a period of 400 nm, and an aspect ratio of 1, and a fine concavo-convex structure having an average diameter of 33 nm and an average height of 33 nm was formed.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件,作為相對於實施例6的比較例,而為比較例5。然後,針對這些實施例6及比較例5的試樣,測定光輸出。將其結果示於第24圖。 The ultraviolet light-emitting semiconductor light-emitting device before the formation of the uneven structure on the substrate was prepared as Comparative Example 5 as a comparative example with respect to Example 6. Then, the light output was measured for the samples of Example 6 and Comparative Example 5. The results are shown in Fig. 24.

請參考第24圖,橫軸是顯示以比較例5為基準的情況之實施例6的光輸出比,縱軸是顯示試樣個數。以比較例5的光輸出為1.00時,實施例6的光輸出比的平均值為1.79。如從第24圖所瞭解,與實施例5同樣在實施例6亦獲得高光輸出比,可顯示具有週期凹凸構造與微細凹凸構造二者的構造的優位性。另外,如從第24圖所瞭解,實施例6的試樣亦與實施例5的試樣同樣顯示其為發光輸出的變異程度相對較小的半導體發 光元件。 Referring to Fig. 24, the horizontal axis is the light output ratio of Example 6 in the case of Comparative Example 5, and the vertical axis is the number of displayed samples. When the light output of Comparative Example 5 was 1.00, the average value of the light output ratio of Example 6 was 1.79. As is understood from Fig. 24, in the same manner as in the fifth embodiment, the high light output ratio was obtained in the sixth embodiment, and the superiority of the structure having both the periodic uneven structure and the fine uneven structure was exhibited. Further, as understood from Fig. 24, the sample of Example 6 was also shown to be a semiconductor having a relatively small variation in luminescence output as in the sample of Example 5. Optical component.

【實施例7】 [Embodiment 7]

基於本發明的上述實施形態相關的半導體發光元件的構造,製作實施例7相關的半導體發光元件。另外,實施例7相關的半導體發光元件的構成,基本上與實施例1中的半導體發光元件同樣。另外,含半導體發光元件的發光層的磊晶層的材料與元件的發光波長是與上述的實施例5同樣。 A semiconductor light-emitting device according to Example 7 was produced based on the structure of the semiconductor light-emitting device according to the above-described embodiment of the present invention. Further, the configuration of the semiconductor light-emitting device of the seventh embodiment is basically the same as that of the semiconductor light-emitting device of the first embodiment. Further, the material of the epitaxial layer of the light-emitting layer including the semiconductor light-emitting element and the light-emitting wavelength of the element were the same as those of the above-described fifth embodiment.

在與已製作的半導體發光元件晶圓的發光元件層為相反的基板面(光取出面),與實施例5同樣藉由電子束描繪,製作蝕刻罩幕圖形。發光部是直徑100μm的圓區域,以發光部的中心為描繪中心,將描繪區域設為900μm×900μm。描繪圖形設為直徑400nm、圖形週期1000nm,圖形排列設正為三角格子排列。其次,與實施例5同樣,在罩幕圖形之上,藉由真空蒸鍍法沉積100nm~500nm的鎳。鎳的沉積後,將半導體發光元件基板浸漬於電子束阻劑的剝離液而移除阻劑及位於此阻劑上的鎳(舉離法)。這麼作,在基板16的背面上形成由鎳構成的罩幕圖形。 An etching mask pattern was produced by electron beam drawing in the same manner as in Example 5 on the substrate surface (light extraction surface) opposite to the light-emitting element layer of the fabricated semiconductor light-emitting device wafer. The light-emitting portion is a circular region having a diameter of 100 μm, and the center of the light-emitting portion is the center of the drawing, and the drawing region is set to 900 μm × 900 μm. The drawing pattern is set to have a diameter of 400 nm and a pattern period of 1000 nm, and the pattern arrangement is set to be a triangular lattice arrangement. Next, in the same manner as in Example 5, nickel of 100 nm to 500 nm was deposited by vacuum evaporation on the mask pattern. After the deposition of nickel, the semiconductor light-emitting device substrate is immersed in the stripping liquid of the electron beam resist to remove the resist and the nickel on the resist (lifting method). In this manner, a mask pattern made of nickel is formed on the back surface of the substrate 16.

接下來,與實施例2同樣,將上述半導體發光元件基板導入ICP蝕刻裝置,使用三氟甲烷(CHF3)氣體施以10分鐘~80分鐘的蝕刻處理。另外,如以實施例5的圖形尺寸較小的構造,則蝕刻處理時間短;相反地如以實施例7的圖形尺寸相對較大的構造,則上述蝕刻處理時間則變長。 Next, in the same manner as in Example 2, the semiconductor light-emitting device substrate was introduced into an ICP etching apparatus, and an etching treatment was performed for 10 minutes to 80 minutes using a trifluoromethane (CHF 3 ) gas. Further, as in the configuration in which the pattern size of the embodiment 5 is small, the etching processing time is short; conversely, in the configuration in which the pattern size of the embodiment 7 is relatively large, the etching processing time becomes long.

最後,為了移除鎳的罩幕圖形,將半導體發光元件基板在已加熱至60℃~90℃的鹽酸浸漬15分鐘。另外,與實 施例2的情況同樣,為了防止半導體發光元件基板的電極金屬因鹽酸而腐蝕,在半導體發光元件基板的電極形成面預先塗佈光阻再使其硬化而作為保護膜使用。浸漬於鹽酸後,以超純水清洗,再以剝離液溶解作為保護膜的光阻。 Finally, in order to remove the mask pattern of nickel, the semiconductor light-emitting device substrate was immersed in hydrochloric acid heated to 60 ° C to 90 ° C for 15 minutes. In addition, and In the case of the second embodiment, in order to prevent the electrode metal of the semiconductor light-emitting device substrate from being corroded by hydrochloric acid, the electrode-forming surface of the semiconductor light-emitting device substrate is coated with a photoresist and then cured to be used as a protective film. After immersing in hydrochloric acid, it was washed with ultrapure water, and the photoresist as a protective film was dissolved in a stripping solution.

藉此,製作具有圓錐底部的直徑1000nm、週期1000nm、高寬比為1的週期凹凸構造與平均直徑33nm、平均高度33nm的微細凹凸構造的基板構成之實施例7的紫外發光的半導體發光元件。 Thus, an ultraviolet light-emitting semiconductor light-emitting device of Example 7 having a periodic concave-convex structure having a diameter of 1000 nm, a period of 1000 nm, and an aspect ratio of 1 and a fine concavo-convex structure having an average diameter of 33 nm and an average height of 33 nm was prepared.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件,作為相對於實施例7的比較例,而為比較例6。然後,針對這些實施例7及比較例6的試樣,測定光輸出。將其結果示於第25圖。 The ultraviolet light-emitting semiconductor light-emitting device before the formation of the uneven structure on the substrate was prepared as Comparative Example 6 as a comparative example with respect to Example 7. Then, the light output was measured for the samples of Example 7 and Comparative Example 6. The results are shown in Fig. 25.

請參考第25圖,橫軸是顯示以比較例6為基準的情況之實施例7的光輸出比,縱軸是顯示試樣個數。以比較例6的光輸出為1.00時,實施例7的光輸出比的平均值為1.69。如從第25圖所瞭解,與實施例5同樣地在實施例7亦獲得高光輸出比,可顯示具有週期凹凸構造與微細凹凸構造二者的構造的優位性。另外,如從第25圖所瞭解,實施例7的試樣亦與實施例5的試樣同樣地顯示其為發光輸出的變異程度相對較小的半導體發光元件。 Referring to Fig. 25, the horizontal axis is the light output ratio of Example 7 in the case of Comparative Example 6, and the vertical axis is the number of displayed samples. When the light output of Comparative Example 6 was 1.00, the average value of the light output ratio of Example 7 was 1.69. As is understood from Fig. 25, in the same manner as in the fifth embodiment, the high light output ratio was obtained in the seventh embodiment, and the superiority of the structure having both the periodic uneven structure and the fine uneven structure was exhibited. Further, as is understood from Fig. 25, the sample of Example 7 was also shown as a semiconductor light-emitting device having a relatively small degree of variation in light-emitting output, similarly to the sample of Example 5.

【實施例8】 [Embodiment 8]

製作將在上述實施例1的半導體發光元件晶圓的光取出面製作的週期凹凸構造(圖形的週期為300nm)的週期設為600nm者,作為實施例8相關的半導體發光元件。另外,為了 將高寬比固定為1,使直徑及高度符合上述圖形週期。另外,上述實施例8相關的半導體發光元件,除了上述圖形週期、直徑及高度以外,全部與實施例1相關的半導體發光元件同樣。另外,製作條件亦是將蝕刻的處理的處理時間設為30分鐘~80分鐘以外,與實施例1同樣。 The period of the periodic uneven structure (the period of the pattern is 300 nm) which is formed on the light extraction surface of the semiconductor light-emitting device wafer of the first embodiment is 600 nm, and is a semiconductor light-emitting device according to the eighth embodiment. In addition, in order Fix the aspect ratio to 1 so that the diameter and height meet the above graphic period. Further, the semiconductor light-emitting device according to the eighth embodiment is the same as the semiconductor light-emitting device according to the first embodiment except for the pattern period, the diameter, and the height. In addition, the production conditions are the same as in the first embodiment except that the processing time of the etching treatment is 30 minutes to 80 minutes.

如此,製作具有圓錐底部的直徑600nm、週期600nm、高度600nm的週期凹凸構造的基板構成之紫外發光的半導體發光元件,作為實施例8相關的半導體發光元件。 In this manner, an ultraviolet light-emitting semiconductor light-emitting device having a substrate having a periodic concave-convex structure of a diameter of 600 nm, a period of 600 nm, and a height of 600 nm having a conical bottom portion was produced as the semiconductor light-emitting device of Example 8.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件,作為相對於實施例8的比較例,而為比較例7。然後,針對此實施例8及比較例7的試樣,測定光輸出。將其結果示於第26圖。 The ultraviolet light-emitting semiconductor light-emitting device before the formation of the uneven structure on the substrate was prepared as Comparative Example 7 as a comparative example with respect to Example 8. Then, the light output was measured for the samples of Example 8 and Comparative Example 7. The results are shown in Fig. 26.

請參考第26圖,橫軸是顯示以比較例7為基準的情況之實施例8的光輸出比,縱軸是顯示試樣個數。以比較例7的光輸出為1.00時,實施例8的光輸出比的平均值為1.44。在此處,比較具有同一週期凹凸構造(週期600nm)的實施例2、實施例8、再加上不具週期凹凸構造的比較例7,光輸出比是依實施例2>實施例8>比較例7的順序遞減,可顯示具有週期凹凸構造與微細凹凸構造二者的構造的優位性。 Referring to Fig. 26, the horizontal axis is the light output ratio of Example 8 in the case of Comparative Example 7, and the vertical axis is the number of displayed samples. When the light output of Comparative Example 7 was 1.00, the average value of the light output ratio of Example 8 was 1.44. Here, Example 2, Example 8 having the same periodic concavo-convex structure (period of 600 nm), and Comparative Example 7 having no periodic concavo-convex structure were compared, and the light output ratio was according to Example 2>Example 8>Comparative Example The order of 7 is decremented, and the superiority of the structure having both the periodic concavo-convex structure and the fine concavo-convex structure can be displayed.

【實施例9】 [Embodiment 9]

製作將在上述實施例1的半導體發光元件晶圓的光取出面製作的週期凹凸構造(圖形的週期為300nm)的週期設為1000nm者,作為實施例9相關的半導體發光元件。另外,為了將高寬比固定為1,使直徑及高度符合上述圖形週期。另外, 上述實施例9相關的半導體發光元件,除了上述圖形週期、直徑及高度以外,全部與實施例1相關的半導體發光元件同樣。另外,製作條件亦是將蝕刻的處理的處理時間設為30分鐘~80分鐘以外,與實施例1同樣。 The period of the periodic uneven structure (the period of the pattern is 300 nm) which is formed on the light extraction surface of the semiconductor light-emitting device wafer of the first embodiment is 1000 nm, and is a semiconductor light-emitting device according to the ninth embodiment. In addition, in order to fix the aspect ratio to 1, the diameter and height are made to conform to the above-described pattern period. In addition, The semiconductor light-emitting device according to the ninth embodiment is the same as the semiconductor light-emitting device according to the first embodiment except for the pattern period, the diameter, and the height. In addition, the production conditions are the same as in the first embodiment except that the processing time of the etching treatment is 30 minutes to 80 minutes.

如此,製作具有圓錐底部的直徑1000nm、週期1000nm、高度1000nm的週期凹凸構造的基板構成之紫外發光的半導體發光元件,作為實施例9相關的半導體發光元件。 In this manner, an ultraviolet light-emitting semiconductor light-emitting device having a substrate having a periodic concave-convex structure of a diameter of 1000 nm, a period of 1000 nm, and a height of 1000 nm having a conical bottom portion was produced as the semiconductor light-emitting device of Example 9.

準備在基板形成凹凸構造前的紫外發光的半導體發光元件,作為相對於實施例9的比較例,而為比較例8。然後,針對此實施例9及比較例8的試樣,測定光輸出。將其結果示於第26圖。 The ultraviolet light-emitting semiconductor light-emitting device before the formation of the uneven structure on the substrate was prepared as Comparative Example 8 as a comparative example with respect to Example 9. Then, the light output was measured for the samples of Example 9 and Comparative Example 8. The results are shown in Fig. 26.

請參考第26圖,橫軸是顯示以比較例8為基準的情況之實施例9的光輸出比,縱軸是顯示試樣個數。以比較例8的光輸出為1.00時,實施例9的光輸出比的平均值為1.26。在此處,比較具有同一週期凹凸構造(週期1000nm)的實施例7、實施例9、再加上不具週期凹凸構造的比較例8,光輸出比是依實施例7>實施例9>比較例8的順序遞減,可顯示具有週期凹凸構造與微細凹凸構造二者的構造的優位性。 Referring to Fig. 26, the horizontal axis is the light output ratio of Example 9 in the case of Comparative Example 8, and the vertical axis is the number of displayed samples. When the light output of Comparative Example 8 was 1.00, the average value of the light output ratio of Example 9 was 1.26. Here, Comparative Example 8 having the same periodic concavo-convex structure (period of 1000 nm), Example 9, and Comparative Example 8 having no periodic concavo-convex structure were compared, and the light output ratio was according to Example 7>Example 9>Comparative Example The order of 8 is decremented, and the superiority of the structure having both the periodic concavo-convex structure and the fine concavo-convex structure can be displayed.

另外,針對上述實施例1、實施例8及實施例9所得的光輸出比,如第27圖所示,與在實施例3所示的計算結果有良好的一致性。這是印證了關於由模擬計算而得的光取出構造的最佳化的方針的妥當性。另外,在第27圖中,是亦組合針對實施例2、實施例5~7所得的光輸出比而描繪。另外,第27圖的橫軸顯示凹凸構造的排列週期(單位:nm)、縱軸顯示光輸出比。 Further, as shown in Fig. 27, the light output ratios obtained in the above-described first embodiment, the eighth embodiment, and the ninth embodiment were in good agreement with the calculation results shown in the third embodiment. This is a proof of the policy of optimizing the light extraction structure obtained by the simulation calculation. Further, in Fig. 27, the light output ratios obtained for Example 2 and Examples 5 to 7 are also combined and drawn. Further, the horizontal axis of Fig. 27 shows the arrangement period (unit: nm) of the uneven structure, and the vertical axis shows the light output ratio.

如同從第27圖亦可瞭解,光輸出比對比於週期凹凸構造的排列週期的傾向,與模擬計算結果幾乎一致。亦即,根據第27圖,印證了光輸出比的絕對值的增加部分,是藉由因微細凹凸構造的附加造成的光取出效率的提升效果的結果。 As can be understood from Fig. 27, the tendency of the light output ratio to compare the arrangement period of the periodic concavo-convex structure is almost identical to the simulation calculation result. In other words, according to Fig. 27, the increase in the absolute value of the light output ratio is confirmed as a result of the effect of improving the light extraction efficiency due to the addition of the fine uneven structure.

本次揭露的實施形態及實施例的全部內容是作為例示,不應認定為限制條件。本發明的範圍並非藉由上述的說明而是藉由申請專利範圍表示,且應包含與申請專利範圍均等的意義及在範圍內的所有變更。 The entire contents of the embodiments and examples disclosed herein are illustrative and should not be construed as limiting. The scope of the present invention is defined by the scope of the claims and the scope of the claims and the scope of the claims.

【產業上的可利用性】 [Industrial availability]

本發明特別有利於應用在發射短波長的光的半導體發光元件。 The present invention is particularly advantageous for use in a semiconductor light emitting element that emits light of a short wavelength.

Claims (14)

一種半導體發光元件,具有含發光層的半導體層,其中上述半導體發光元件的表面包含光取出面;上述光取出面及上述半導體發光元件內折射率互異的二層的界面的至少任一個,包括:週期凹凸構造,具有比從上述發光層發射的光的波長的0.5倍還大的週期;以及微細凹凸構造,位於上述週期凹凸構造的表面上且在上述週期凹凸構造的凹部上分布得比在上述週期凹凸構造的凸部上還要密集,上述微細凹凸構造具有上述光的波長的0.5倍以下的平均直徑。 A semiconductor light-emitting device having a semiconductor layer including a light-emitting layer, wherein a surface of the semiconductor light-emitting device includes a light extraction surface; and at least one of an interface between the light extraction surface and the semiconductor light-emitting device having a refractive index different from each other includes a periodic concavo-convex structure having a period larger than 0.5 times a wavelength of light emitted from the light-emitting layer; and a fine concavo-convex structure located on a surface of the periodic concavo-convex structure and distributed over the concave portion of the periodic concavo-convex structure The convex portion of the periodic concavo-convex structure is densely formed, and the fine concavo-convex structure has an average diameter of 0.5 times or less of the wavelength of the light. 一種半導體發光元件,具有含發光層的半導體層,其中上述半導體發光元件的表面包含光取出面;上述光取出面及上述半導體發光元件內折射率互異的二層的界面的至少任一個,包括:週期凹凸構造,具有比從上述發光層發射的光的波長還大的週期;以及微細凹凸構造,位於上述週期凹凸構造的表面上且具有上述光的波長的0.5倍以下的平均直徑;以及從上述發光層發射的光的波長為350nm以下。 A semiconductor light-emitting device having a semiconductor layer including a light-emitting layer, wherein a surface of the semiconductor light-emitting device includes a light extraction surface; and at least one of an interface between the light extraction surface and the semiconductor light-emitting device having a refractive index different from each other includes a periodic concavo-convex structure having a period larger than a wavelength of light emitted from the light-emitting layer; and a fine concavo-convex structure having an average diameter of 0.5 times or less of a wavelength of the light on a surface of the periodic concavo-convex structure; The light emitted from the light-emitting layer has a wavelength of 350 nm or less. 如申請專利範圍第1或2項所述的半導體發光元件,其中上述週期凹凸構造的排列圖形為三角格子狀。 The semiconductor light-emitting device according to claim 1 or 2, wherein the arrangement pattern of the periodic uneven structure is a triangular lattice shape. 如申請專利範圍第1或2項所述的半導體發光元件,其中上述週期凹凸構造包含折射率高於空氣的高折射率材料部;在對於從上述發光層向上述光取出面的方向垂直的面的上 述高折射率材料部的截面積,是隨著遠離上述發光層而變小。 The semiconductor light-emitting device according to claim 1 or 2, wherein the periodic uneven structure includes a high refractive index material portion having a refractive index higher than air; and a surface perpendicular to a direction from the light emitting layer toward the light extraction surface On The cross-sectional area of the high refractive index material portion is smaller as it goes away from the light-emitting layer. 如申請專利範圍第4項所述的半導體發光元件,其中上述高折射率材料部包含由折射率高於空氣的高折射率材料構成的凸部;上述凸部的形狀為錐體形狀或半橢圓球形狀。 The semiconductor light-emitting device of claim 4, wherein the high refractive index material portion comprises a convex portion composed of a high refractive index material having a refractive index higher than air; and the convex portion has a pyramid shape or a semi-elliptical shape. Ball shape. 如申請專利範圍第1或2項所述的半導體發光元件,其中上述發光層含III族氮化物半導體;上述半導體層含:導電型為n型的n型III族氮化物半導體層;以及導電型為p型的p型III族氮化物半導體層,位於從上述發光層所見與上述n型III族氮化物半導體層的相反側。 The semiconductor light-emitting device according to claim 1 or 2, wherein the light-emitting layer contains a group III nitride semiconductor; and the semiconductor layer comprises: an n-type group III nitride semiconductor layer of a conductivity type; and a conductive type The p-type p-type group III nitride semiconductor layer is located on the opposite side of the above-described n-type group III nitride semiconductor layer as seen from the above-mentioned light-emitting layer. 如申請專利範圍第1或2項所述的半導體發光元件,其具有一透明性基板,配置於從上述發光層到上述光取出面側,對從上述發光層發射的光具有透明性。 The semiconductor light-emitting device according to claim 1 or 2, further comprising a transparent substrate disposed on the side of the light-emitting layer from the light-emitting layer and having transparency to light emitted from the light-emitting layer. 如申請專利範圍第7項所述的半導體發光元件,其中上述透明性基板為氮化鋁基板。 The semiconductor light-emitting device according to claim 7, wherein the transparent substrate is an aluminum nitride substrate. 如申請專利範圍第1項所述的半導體發光元件,其中從上述發光層發射的光的波長為450nm以下。 The semiconductor light-emitting device according to claim 1, wherein the light emitted from the light-emitting layer has a wavelength of 450 nm or less. 如申請專利範圍第1或2項所述的半導體發光元件,其中上述週期凹凸構造的高度相對於上述週期凹凸構造的週期為1/3倍以上、5倍以下;上述微細凹凸構造的平均高度相對於上述微細凹凸構造的上述平均直徑為0.1倍以上、10倍以下。 The semiconductor light-emitting device according to the first or second aspect, wherein the height of the periodic concavo-convex structure is 1/3 times or more and 5 times or less with respect to a period of the periodic concavo-convex structure; and an average height of the fine concavo-convex structure is relatively The average diameter of the fine concavo-convex structure is 0.1 times or more and 10 times or less. 如申請專利範圍第1項所述的半導體發光元件,其中從上述發光層發射的光的波長為350nm以下;以及上述週期凹凸構造的週期大於從上述發光層發射的光的波長。 The semiconductor light-emitting device according to claim 1, wherein a wavelength of light emitted from the light-emitting layer is 350 nm or less; and a period of the periodic uneven structure is larger than a wavelength of light emitted from the light-emitting layer. 一種半導體發光元件的製造方法,包含:準備即將成為包含具有發光層的半導體層的半導體發光元件的元件構件;在上述元件構件之形成上述半導體發光元件的光取出面的區域上,形成具有圖形的罩幕層;以及以上述罩幕層為罩幕,藉由蝕刻部分性地移除形成上述光取出面的上述區域,藉此形成週期凹凸構造;其中上述罩幕層為金屬罩幕層;在上述週期凹凸構造的形成中,是藉由進行使用氟系氣體作為蝕刻氣體的乾蝕刻,形成上述週期凹凸構造,並在上述週期凹凸構造的表面形成微細凹凸構造;上述週期凹凸構造,具有超過從上述發光層發射的光的波長的0.5倍的週期;上述微細凹凸構造具有上述光的波長的0.5倍以下的平均直徑;上述週期凹凸構造的形成,包含:進行上述乾蝕刻及移除上述金屬罩幕層;上述週期凹凸構造的週期與上述金屬罩幕層的週期相同;在進行上述乾蝕刻中,上述金屬罩幕層與上述蝕刻氣體的反應物附著於形成上述光取出面的上述區域;以及 在移除上述金屬罩幕層中,是藉由酸處理移除上述金屬罩幕層。 A method of manufacturing a semiconductor light-emitting device, comprising: preparing an element member to be a semiconductor light-emitting element including a semiconductor layer having a light-emitting layer; and forming a pattern on a region of the element member on which a light extraction surface of the semiconductor light-emitting element is formed a mask layer; and the mask layer is used as a mask to partially remove the region forming the light extraction surface by etching, thereby forming a periodic uneven structure; wherein the mask layer is a metal mask layer; In the formation of the periodic concavo-convex structure, the periodic concavo-convex structure is formed by dry etching using a fluorine-based gas as an etching gas, and a fine concavo-convex structure is formed on the surface of the periodic concavo-convex structure; a period of 0.5 times a wavelength of light emitted from the light-emitting layer; the fine uneven structure having an average diameter of 0.5 times or less of a wavelength of the light; and the forming of the periodic uneven structure includes: performing the dry etching and removing the metal cover Curtain layer; the period of the above-mentioned periodic concave-convex structure and the above-mentioned metal mask layer Of the same; the dry etching is performed, the reaction product of the metal mask layer and the etching gas is adhered to form the region of the light extraction surface; and In removing the above metal mask layer, the above metal mask layer is removed by an acid treatment. 如申請專利範圍第12項所述的半導體發光元件的製造方法,其中上述金屬罩幕層包含一鎳膜。 The method of manufacturing a semiconductor light-emitting device according to claim 12, wherein the metal mask layer comprises a nickel film. 如申請專利範圍第12或13項所述的半導體發光元件的製造方法,其中上述蝕刻氣體包含含碳的氟系氣體。 The method for producing a semiconductor light-emitting device according to claim 12, wherein the etching gas contains a fluorine-containing gas containing carbon.
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